From c766c368e8f3c172ab61bdf27d7d85b6ca6db797 Mon Sep 17 00:00:00 2001 From: Hunter Date: Thu, 24 Jul 2025 10:38:05 -0400 Subject: [PATCH 01/11] initial steps --- radbase/converter.py | 36 ++++++++++++++++-------------------- radbase/radius_analyzer.py | 17 +++++------------ 2 files changed, 21 insertions(+), 32 deletions(-) diff --git a/radbase/converter.py b/radbase/converter.py index 75d6040..4a0c9bd 100644 --- a/radbase/converter.py +++ b/radbase/converter.py @@ -1,36 +1,32 @@ -from abc import ABC, abstractmethod +from abc import ABC +from .radius_analyzer import RadiiInformation -class Measurement(ABC): - - @abstractmethod - def calc_radius(self, information): - pass - @abstractmethod - def calc_seltzer(self): - pass +class ConversionStep(ABC): + pass -class MuonicMeasurement(Measurement): +class ConversionStrategy: pass -class ElectronicMeasurement(Measurement): - pass +class ConversionRecord: + def __init__(self): + pass -class KalphaMeasurement(Measurement): - pass +class Measurement(ABC): + + def __init__(self): + pass -class OISMeasurement(Measurement): - pass +class Converter: -class RadiusConverter: - measurements = list[Measurement] + def __init__(self, conversion_strategy: ConversionStrategy): + self.strategy = conversion_strategy - def request_information(self, information): - """Retrieves desired quantity from measurements; if quantity not found yields a calculated value""" + def convert(self, measurements: list[Measurement], conversion_steps) -> RadiiInformation: # or something like RI pass diff --git a/radbase/radius_analyzer.py b/radbase/radius_analyzer.py index b6dd254..46273b6 100644 --- a/radbase/radius_analyzer.py +++ b/radbase/radius_analyzer.py @@ -13,6 +13,8 @@ from lmfit import Minimizer, Parameters from uncertainties import correlated_values_norm, correlation_matrix, ufloat +from .converter import Measurement + class Nuclide: z: int @@ -180,8 +182,9 @@ class RadiusData: data_id: int correlations: defaultdict[int, dict] nuclides: list[Nuclide] + measurement: None | Measurement - def __init__(self, term: str | Term, value, unc, data_id, **kwargs): + def __init__(self, term: str | Term, value, unc, data_id, measurement=None, **kwargs): if isinstance(term, Term): self.term = term elif isinstance(term, str): @@ -194,6 +197,7 @@ def __init__(self, term: str | Term, value, unc, data_id, **kwargs): self.data_id = data_id self.correlations = defaultdict(dict) self.nuclides = self.term.get_nuclides() + self.measurement = measurement def residual(self, params, normalize=True): resid = self.term.eval(params=params) - self.value @@ -208,17 +212,6 @@ def __repr__(self): return f'Id {self.data_id}: {self.term.termstr} = {self.value} +/- {self.unc}' -class Measurement(RadiusData): - - def __init__(self, references, **kwargs): - super().__init__(**kwargs) - self.references = references - - @abstractmethod - def calc_radius(self): - pass - - class Projection(RadiusData): connected_measurements = list[Measurement] From 4585dbe70ff9d5396bc9972758b9d5b0242c2e4f Mon Sep 17 00:00:00 2001 From: Hunter Date: Sat, 31 Jan 2026 15:35:03 -0500 Subject: [PATCH 02/11] Added DataEntryInterface and template systems. Entered Ke75 and Be88. --- .pre-commit-config.yaml | 1 + .../Muonic Barrett Moment.json | 110 ++ .../bergem_nuclear_1988/Muonic Radius.json | 46 + .../Muonic Transition Energy.json | 182 +++ .../compilation/bergem_nuclear_1988/notes.txt | 1 + .../Fermi Distribution.json | 126 ++ .../kessler_muonic_1975/Muonic Radius.json | 58 + ...gy Difference (different transitions).json | 658 +++++++++ .../Muonic Transition Energy.json | 834 ++++++++++++ radbase/compilation/references.json | 70 + .../Muonic Transition Energy.json | 110 ++ radbase/converter.py | 141 +- radbase/data_entry.py | 1203 +++++++++++++++++ radbase/radius_analyzer.py | 35 +- tests/test_converter.py | 4 + tests/test_data_entry.py | 150 ++ 16 files changed, 3684 insertions(+), 45 deletions(-) create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Radius.json create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json create mode 100644 radbase/compilation/bergem_nuclear_1988/notes.txt create mode 100644 radbase/compilation/kessler_muonic_1975/Fermi Distribution.json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Radius.json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Transition Energy.json create mode 100644 radbase/compilation/references.json create mode 100644 radbase/compilation/test_test_1700/Muonic Transition Energy.json create mode 100644 radbase/data_entry.py create mode 100644 tests/test_converter.py create mode 100644 tests/test_data_entry.py diff --git a/.pre-commit-config.yaml b/.pre-commit-config.yaml index 4ab80ef..4a1baf6 100644 --- a/.pre-commit-config.yaml +++ b/.pre-commit-config.yaml @@ -19,6 +19,7 @@ repos: hooks: - id: flake8 additional_dependencies: [flake8-deprecated, flake8-mutable, Flake8-pyproject] + exclude: tests/ - repo: https://github.com/PyCQA/isort/ rev: 5.13.2 diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json b/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json new file mode 100644 index 0000000..0699bf7 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json @@ -0,0 +1,110 @@ +{ + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.8821(6)", + "k [-]": "1.1456", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "-2.136E-5", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9370(3)", + "k [-]": "1.3993", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "-1.268E-5", + "Notes": "" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9960(3)", + "k [-]": "1.8474", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "8.547E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9958(4)", + "k [-]": "1.8715", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "7.909E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.0319(1)", + "k [-]": "2.2429", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.478E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.0320(1)", + "k [-]": "2.2559", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.406E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1222(3)", + "k [-]": "3.4781", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "9.128E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1654(9)", + "k [-]": "4.0454", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.329E-5", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1670(4)", + "k [-]": "4.0699", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.318E-5", + "Notes": "Experimental Uncertainty Only" + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json b/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json new file mode 100644 index 0000000..4e3796a --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json @@ -0,0 +1,46 @@ +{ + "bergem_nuclear_1988_radius_Pb208_NP_Calculated": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.504, + "uncertainty": 0.0011 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 187.0, + "Notes": "Fixed alpha=0.1415 from e- scattering" + }, + "bergem_nuclear_1988_radius_Pb208_NP_Fit": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.5031, + "uncertainty": 0.0011 + }, + "Nuclear Polarization Method": "Fit", + "Reduced Chi-Squared": 0.19, + "Notes": "Alpha=0.1415, 2pf fit, " + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json b/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json new file mode 100644 index 0000000..e929040 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json @@ -0,0 +1,182 @@ +{ + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": "5962.854(90)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": "5778.058(100)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": "2642.332(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "2500.590(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "2457.569(70)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": "1507.754(50)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p1/2", + "Lower": "2s1/2" + }, + "Energy [keV]": "1460.558(32)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": "1215.330(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "1030.543(27)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": "1404.659(20)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "1366.347(19)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "1361.748(250)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": "971.974(17)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "938.096(18)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "928.883(14)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d3/2", + "Lower": "3p1/2" + }, + "Energy [keV]": "920.959(28)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d5/2", + "Lower": "3p3/2" + }, + "Energy [keV]": "891.383(22)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d3/2", + "Lower": "3p3/2" + }, + "Energy [keV]": "873.761(63)", + "Notes": "" + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/notes.txt b/radbase/compilation/bergem_nuclear_1988/notes.txt new file mode 100644 index 0000000..cf57e62 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/notes.txt @@ -0,0 +1 @@ +TODO: Add the correlations between transition energies from Table VI diff --git a/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json b/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json new file mode 100644 index 0000000..b95e42c --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json @@ -0,0 +1,126 @@ +{ + "kessler_muonic_1975_fermi_Pb208": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2" + ], + "Nuclide": "Pb208", + "c [fm]": { + "value": 6.65, + "uncertainty": 0.007 + }, + "a [fm]": { + "value": 0.526, + "uncertainty": 0.0014 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb207": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2" + ], + "Nuclide": "Pb207", + "c [fm]": { + "value": 6.647, + "uncertainty": 0.005 + }, + "a [fm]": { + "value": 0.523, + "uncertainty": 0.003 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb206": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2" + ], + "Nuclide": "Pb206", + "c [fm]": { + "value": 6.649, + "uncertainty": 0.019 + }, + "a [fm]": { + "value": 0.517, + "uncertainty": 0.01 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb204": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2" + ], + "Nuclide": "Pb204", + "c [fm]": { + "value": 6.627, + "uncertainty": 0.014 + }, + "a [fm]": { + "value": 0.52, + "uncertainty": 0.008 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + } +} diff --git a/radbase/compilation/kessler_muonic_1975/Muonic Radius.json b/radbase/compilation/kessler_muonic_1975/Muonic Radius.json new file mode 100644 index 0000000..be5870a --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Muonic Radius.json @@ -0,0 +1,58 @@ +{ + "kessler_muonic_1975_radius_Pb204_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb204" + ], + "Nuclide": "Pb204", + "R [fm]": { + "value": 5.4857, + "uncertainty": 0.0012 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.47, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb206_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb206" + ], + "Nuclide": "Pb206", + "R [fm]": { + "value": 5.497, + "uncertainty": 0.0015 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.73, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb208_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb208" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.5097, + "uncertainty": 0.0006 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.11, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb207_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb207" + ], + "Nuclide": "Pb207", + "R [fm]": { + "value": 5.5036, + "uncertainty": 0.0004 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.05, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + } +} diff --git a/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json b/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json new file mode 100644 index 0000000..bbd091c --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json @@ -0,0 +1,658 @@ +{ + "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 184.83, + "uncertainty": 0.01 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.09, + "uncertainty": 0.14 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.75, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 186.04, + "uncertainty": 0.11 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 141.77, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 141.82, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 142.53, + "uncertainty": 0.05 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 142.68, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 184.89, + "uncertainty": 0.25 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.05, + "uncertainty": 0.17 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.76, + "uncertainty": 0.4 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.82, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_3d5/2_2p3/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.13, + "uncertainty": 0.18 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_3d5/2_2p3/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.25, + "uncertainty": 0.13 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_3d5/2_2p3/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.24, + "uncertainty": 0.36 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_3d5/2_2p3/2_B_3d3/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "B": { + "Upper": "3d3/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.13, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "4f5/2", + "Lower": "4f7/2" + }, + "C": { + "Upper": "4f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.07, + "uncertainty": 0.03 + }, + "Notes": "Using 4f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "4f5/2", + "Lower": "4f7/2" + }, + "C": { + "Upper": "4f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.2, + "uncertainty": 0.03 + }, + "Notes": "Using 4f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "4f5/2", + "Lower": "4f7/2" + }, + "C": { + "Upper": "4f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.19, + "uncertainty": 0.03 + }, + "Notes": "Using 4f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "4f5/2", + "Lower": "4f7/2" + }, + "C": { + "Upper": "4f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.08, + "uncertainty": 0.03 + }, + "Notes": "Using 4f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "5f5/2", + "Lower": "5f7/2" + }, + "C": { + "Upper": "5f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 42.95, + "uncertainty": 0.1 + }, + "Notes": "Using 5f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "5f5/2", + "Lower": "5f7/2" + }, + "C": { + "Upper": "5f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 42.98, + "uncertainty": 0.09 + }, + "Notes": "Using 5f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "5f5/2", + "Lower": "5f7/2" + }, + "C": { + "Upper": "5f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 42.95, + "uncertainty": 0.1 + }, + "Notes": "Using 5f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "5f5/2", + "Lower": "5f7/2" + }, + "C": { + "Upper": "5f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 42.84, + "uncertainty": 0.14 + }, + "Notes": "Using 5f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "6f5/2", + "Lower": "6f7/2" + }, + "C": { + "Upper": "6f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.04, + "uncertainty": 0.24 + }, + "Notes": "Using 6f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "6f5/2", + "Lower": "6f7/2" + }, + "C": { + "Upper": "6f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.28, + "uncertainty": 0.31 + }, + "Notes": "Using 6f splitting from theory" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "B": { + "Upper": "6f5/2", + "Lower": "6f7/2" + }, + "C": { + "Upper": "6f7/2", + "Lower": "3d5/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 43.24, + "uncertainty": 0.36 + }, + "Notes": "Using 6f splitting from theory" + }, + 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"Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.67, + "uncertainty": 0.15 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.68, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.11, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.8, + "uncertainty": 0.19 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1639.98, + "uncertainty": 0.19 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1640.23, + "uncertainty": 0.24 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1639.92, + "uncertainty": 0.24 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1640.21, + "uncertainty": 0.34 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1030.44, + "uncertainty": 0.17 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1030.02, + "uncertainty": 0.27 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1029.99, + "uncertainty": 0.41 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1028.83, + "uncertainty": 0.38 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.43, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.6, + "uncertainty": 0.45 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.58, + "uncertainty": 0.54 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1214.12, + "uncertainty": 0.3 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1507.48, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1508.71, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1509.53, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1511.63, + "uncertainty": 0.2 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json new file mode 100644 index 0000000..a82f481 --- /dev/null +++ b/radbase/compilation/references.json @@ -0,0 +1,70 @@ +{ + "zehnder_charge_1975": { + "title": "CHARGE PARAMETERS, ISOTOPE SHIFTS, QUADRUPOLE MOMENTS, AND NUCLEAR EXCITATION IN MUONIC 170-174, 176yb", + "author": [ + "A. Zehnder", + "F. Boehm", + "W. Dey", + "R. Engfer", + "H. K. Walter", + "J. L. Vuilleumier" + ], + "year": "1975", + "month": null, + "journal": "Nuclear Physics A", + "volume": 254, + "pages": "315-340", + "url": "https://www.sciencedirect.com/science/article/abs/pii/0375947475902195", + "doi": "10.1016/0375-9474(75)90219-5" + }, + "bergem_nuclear_1988": { + "title": "Nuclear polarization and charge moments of \n208 Pb from muonic x rays", + "author": [ + "P. Bergem", + "G. Piller", + "A. Rueetschi", + "L. A. Schaller", + "L. Schellenberg", + "H. Schneuwly" + ], + "year": "1988", + "month": "June", + "journal": "Physical Review C", + "volume": "37", + "pages": "2821", + "url": "https://journals.aps.org/prc/abstract/10.1103/PhysRevC.37.2821", + "doi": "10.1103/PhysRevC.37.2821" + }, + "kessler_muonic_1975": { + "title": "Muonic x rays in lead isotopes", + "author": [ + "D. Kessler", + "H. Mes", + "A. C. Thompson", + "H. L. Anderson", + "M. S. Dixit", + "C. K. Hargrove", + "R. J. McKee" + ], + "year": "1975", + "month": "May", + "journal": "Physical Review C", + "volume": "11", + "pages": "1719-1734", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.11.1719", + "doi": "10.1103/PhysRevC.11.1719" + }, + "test_test_1700": { + "title": "Test", + "author": [ + "Test Test" + ], + "year": "1700", + "month": null, + "journal": null, + "volume": "", + "pages": "", + "url": null, + "doi": null + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy.json b/radbase/compilation/test_test_1700/Muonic Transition Energy.json new file mode 100644 index 0000000..f527937 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy.json @@ -0,0 +1,110 @@ +{ + "test_test_1700_muonic_Pb204_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 300.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb203_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb203", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 200.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb203_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb203", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 100.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb204_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 400.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb200_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb200", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 202.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb200_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb200", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 203.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb100_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb100", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 102.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb100_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb100", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 103.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/converter.py b/radbase/converter.py index 4a0c9bd..3706aa0 100644 --- a/radbase/converter.py +++ b/radbase/converter.py @@ -1,32 +1,151 @@ -from abc import ABC +""" +Measurement -> ConvertedQuantity -> ... -> Radius -from .radius_analyzer import RadiiInformation +TODO: Consider better way of defining the type of a quantity. For example, each quantity will have a value and an +uncertainty, and then some kind of identifier (just a string?) for what those numbers go with. For now, I will use the +naive approach of using strings, although this will definitely come back to haunt me. +""" +from abc import ABC, abstractmethod +from dataclasses import dataclass, field +from typing import Callable, Literal, Tuple -class ConversionStep(ABC): - pass +from uncertainties import UFloat, ufloat +# from .radius_analyzer import Nuclide -class ConversionStrategy: - pass +# from .radius_analyzer import RadiiInformation -class ConversionRecord: +class Nuclide: + z: int + a: int - def __init__(self): - pass + def __init__(self, nucstr): + self.nucstr = nucstr + nucstr = nucstr[1:] + self.z = int(nucstr[:3]) + self.a = int(nucstr[3:]) + self.n = self.a - self.z + + def guess_radius(self): + # semiempirical estimate + return (0.9071 + 1.1025 / (self.a ** (2 / 3)) + -0.548 / (self.a ** (4 / 3))) * self.a ** (1 / 3) + + def __repr__(self): + return f'Nuclide (Z={self.z}, A={self.a})' + + def __eq__(self, other): + return (self.z == other.z) and (self.a == other.a) + + def __lt__(self, other): + if self.z != other.z: + return self.z < other.z + return self.a < other.a + + def __hash__(self): + return self.z * 1000 + self.a + def __str__(self): + return f'R{self.z:03}{self.a:03}' -class Measurement(ABC): + +class Transition: def __init__(self): + raise NotImplementedError() + + +class QuantityType(str): + pass + + +@dataclass +class Quantity: + uvar: UFloat + value: float = field(init=False) + unc: float = field(init=False) + unit: str + quantity: QuantityType + + def __post_init__(self): + self.value = self.uvar.n + self.unc = self.uvar.s + + +class MuonicTransitionEnergyMeasurement: + reference: str + transition: Transition + nuclide: Nuclide + uvar: UFloat + unit: Literal['eV'] + + +class OpticalIsotopeShiftMeasurement: + reference: str + transition: Transition + nuclide_heavier: Nuclide + nuclide_lighter: Nuclide + uvar: UFloat + unit: Literal['THz'] + + +@dataclass +class ConversionHistory: + + """Stores one step of how a converted quantity was obtained. Contains input quantites and ConverstionStep(s) followed + to reach the ConvertedQuantity. By following the chain of ConversionHistories, the full conversion process can + be reconstructed.""" + + conversion_text: str + input_quantities: Tuple[Quantity] + output_quantity: Quantity + conversion_func: Callable | None + + +@dataclass +class Measurement(Quantity): + ref: str | None + + +@dataclass +class ConvertedQuantity(Quantity): + history: ConversionHistory + + +class ConversionStep(ABC): + """ + Wrapper around a conversion function that indicates input data types, creates the conversion history for the output, + and returns the output type. + """ + + input_quantities: tuple[QuantityType] + output_quantity: QuantityType + conversion_function: Callable[[*Tuple[ufloat]], ufloat] # Variable number of ufloats as input, returns ufloat as output + + def __init__(self, input_quantities: tuple[QuantityType], output_quantity: QuantityType, + conversion_function: Callable[[*Tuple[ufloat]], ufloat]): + self.input_quantities = input_quantities + self.output_quantity = output_quantity + self.conversion_function = conversion_function + + @abstractmethod + def convert_quantity(self, *inputs) -> ConvertedQuantity: + pass + + @abstractmethod + def create_history(self, *inputs) -> ConversionHistory: pass +class ConversionStrategy: + pass + + class Converter: def __init__(self, conversion_strategy: ConversionStrategy): self.strategy = conversion_strategy - def convert(self, measurements: list[Measurement], conversion_steps) -> RadiiInformation: # or something like RI + def convert(self, measurements: list[Measurement], conversion_steps: list[Quantity]): # or something like RI pass diff --git a/radbase/data_entry.py b/radbase/data_entry.py new file mode 100644 index 0000000..48546e6 --- /dev/null +++ b/radbase/data_entry.py @@ -0,0 +1,1203 @@ +""" +A simple UI to assist with the compilation of previous nuclear radius information. +""" + +import json +import re +import tkinter as tk +from collections import OrderedDict +from dataclasses import dataclass +from importlib.resources import files +from importlib.resources.abc import Traversable +from pathlib import Path +from tkinter import messagebox, scrolledtext, ttk +from typing import Any, Callable, Literal, NamedTuple, Optional, Protocol + +import uncertainties + +config = { + 'compilation_dir': files('radbase') / 'compilation', + 'reference_path': files('radbase') / 'compilation/references.json' +} + + +@dataclass +class Reference: + title: str + author: list[str] + year: str + month: Optional[str] = None + journal: Optional[str] = None + pages: Optional[int] = None + volume: Optional[int] = None + url: Optional[str] = None + doi: Optional[str] = None + + +class ToolTip: + def __init__(self, widget, text: str, delay: int = 500): + self.widget = widget + self.text = text + self.delay = delay + self._after_id = None + self._tip = None + + widget.bind("", self._schedule) + widget.bind("", self._hide) + widget.bind("", self._hide) + + def _schedule(self, _): + self._after_id = self.widget.after(self.delay, self._show) + + def _show(self): + if self._tip or not self.text: + return + + x = self.widget.winfo_rootx() + 20 + y = self.widget.winfo_rooty() + self.widget.winfo_height() + 5 + + self._tip = tk.Toplevel(self.widget) + self._tip.wm_overrideredirect(True) + self._tip.wm_geometry(f"+{x}+{y}") + + label = ttk.Label( + self._tip, + text=self.text, + background="#ffffe0", + relief="solid", + borderwidth=1, + padding=6, + wraplength=300 + ) + label.pack() + + def _hide(self, _=None): + if self._after_id: + self.widget.after_cancel(self._after_id) + self._after_id = None + if self._tip: + self._tip.destroy() + self._tip = None + + +class FieldProcessor(Protocol): + def process(self, widget: tk.Widget) -> Any: + pass + + +class CastProcessor: + + def __init__(self, field_type: type, allows_empty: bool = False): + self.field_type = field_type + self.allows_empty = allows_empty + + def process(self, widget: tk.Widget): + raw = widget.get() + if raw == "" and not self.allows_empty: + raise ValueError("Field is empty") + return self.field_type(raw) + + +class NumberWithUncertaintyProcessor: + + @staticmethod + def process(widget: tk.Widget): + raw = widget.get().strip() + try: + value = float(raw) + return {'value': value, 'uncertainty': None} + except ValueError: + try: + uvar = uncertainties.ufloat_fromstr(raw) + return {'value': uvar.n, 'uncertainty': uvar.s} + except ValueError: + raise ValueError( + f'Entered value of {raw} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') + + +class MultiTransitionProcessor: + @staticmethod + def process(widget: tk.Widget): + data = {} + for label, container in widget.transition_entries: + data[label.cget("text")] = TransitionProcessor().process(container) + return data + + +class NuclideProcessor: + @staticmethod + def process(widget: tk.Widget): + raw = widget.get() + if re.match(r'[a-zA-Z]{2}\d{1,3}', raw): + return raw + elif re.match(r'[a-zA-Z]{2}nat', raw): + return raw + else: + raise ValueError( + 'Entered Nuclide does not match pattern of two letters and one to three numbers (Ex. Pb208') + + +class ReferenceProcessor: + def __init__(self, reference_path: Traversable): + self.reference_path = reference_path + + @property + def references(self): + pass + + @references.getter + def references(self): + with open(self.reference_path, 'r') as f: + return json.load(f) + + def process(self, widget: tk.Widget): + value = widget.get().strip() + + if value not in sorted(self.references.keys()): + raise ValueError( + f"Reference '{value}' is not a known citation key" + ) + + return value + + +class SelectProcessor: + def __init__(self, options: list[str]): + self.options = set(options) + + def process(self, widget: tk.Widget) -> str: + value = widget.get().strip() + + if not value: + raise ValueError("No option selected") + + if value not in self.options: + raise ValueError(f"'{value}' is not a valid selection") + + return value + + +class TransitionProcessor: + SIMPLE_LEVEL_PATTERN = re.compile( + r""" + ^ + \d+ # principal quantum number + [spdf] # orbital + (\d+/\d+)? # optional j (e.g. 3/2) + $ + """, + re.VERBOSE + ) + + HYBRID_LEVEL_PATTERN = re.compile( + r""" + ^ + \d+[+-] # nuclear spin/parity (e.g. 2+, 0-) + , + \d+ # principal quantum number + [spdf] # orbital + \d+/\d+ # required j + $ + """, + re.VERBOSE + ) + + def process(self, widget: tk.Widget) -> dict[str, str]: + upper = widget.upper_entry.get().strip() + lower = widget.lower_entry.get().strip() + + if not upper or not lower: + raise ValueError("Both upper and lower transition levels must be provided") + + upper_simple = self.SIMPLE_LEVEL_PATTERN.match(upper) + lower_simple = self.SIMPLE_LEVEL_PATTERN.match(lower) + + upper_hybrid = self.HYBRID_LEVEL_PATTERN.match(upper) + lower_hybrid = self.HYBRID_LEVEL_PATTERN.match(lower) + + # both simple or both hybrid + if upper_simple and lower_simple or upper_hybrid and lower_hybrid: + return {'Upper': upper, 'Lower': lower} + + raise ValueError( + "Invalid transition format.\n" + "Both levels must be either:\n" + " - Simple atomic levels (e.g. 2p3/2)\n" + " - Hybrid nuclear+atomic levels (e.g. 2+,1s1/2)" + ) + + +class PreviousMeasurementProcessor: + @staticmethod + def process(widget: tk.Widget) -> list[str]: + selected = [ + key + for key, var in widget.selection_vars.items() + if var.get() + ] + if not selected: + raise ValueError("At least one previous measurement must be selected") + return selected + + +class Widgetcreator(Protocol): + def create_widget(self, frame, row) -> tk.Widget: + pass + + +class DefaultWidgetcreator: + @staticmethod + def create_widget(frame, row) -> tk.Widget: + entry = ttk.Entry(frame, width=40) + entry.grid(row=row, column=1, pady=4, sticky='w') + return entry + + +class PreviousMeasurementWidgetCreator: + + def __init__(self, compilation_path: Traversable, filter_regex: str = ""): + self.filter_regex = filter_regex + self.previous_measurements = self.load_previous_measurements_from_json(compilation_path) + + @staticmethod + def load_previous_measurements_from_json(compilation_path: Traversable) -> list[str]: + previous_measurements = [] + for reference_dir in compilation_path.iterdir(): + if not reference_dir.is_dir(): + continue + for json_file in reference_dir.iterdir(): + if '.json' not in str(json_file): + continue + with open(json_file, "r", encoding="utf-8") as f: + previous_measurements.extend(json.load(f).keys()) + + return sorted(previous_measurements) + + # CHATGPT generated. TODO: Double check this works as intended. + def create_widget(self, frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + # --- filter entry --- + filter_var = tk.StringVar() + filter_var.set(self.filter_regex) + filter_entry = ttk.Entry(container, width=40, textvariable=filter_var) + filter_entry.grid(row=0, column=0, columnspan=2, sticky="w") + + # --- scrollable checklist --- + canvas = tk.Canvas(container, height=150) + scrollbar = ttk.Scrollbar(container, orient="vertical", command=canvas.yview) + checklist_frame = ttk.Frame(canvas) + + canvas.configure(yscrollcommand=scrollbar.set) + + canvas.grid(row=1, column=0, sticky="nsew") + scrollbar.grid(row=1, column=1, sticky="ns") + + canvas.create_window((0, 0), window=checklist_frame, anchor="nw") + + # --- checkbox state --- + vars_by_key: dict[str, tk.BooleanVar] = {} + checkbox_widgets: dict[str, ttk.Checkbutton] = {} + + for data_key in self.previous_measurements: + var = tk.BooleanVar(value=False) + check = ttk.Checkbutton( + checklist_frame, + text=data_key, + variable=var + ) + check.pack(anchor="w") + vars_by_key[data_key] = var + checkbox_widgets[data_key] = check + + def update_scrollregion(*_): + canvas.configure(scrollregion=canvas.bbox("all")) + + checklist_frame.bind("", update_scrollregion) + + # --- regex filtering logic --- + def filter_list(*_): + pattern = filter_var.get() + try: + regex = re.compile(pattern, re.IGNORECASE) + except re.error: + # Invalid regex: hide everything + for chk in checkbox_widgets.values(): + chk.pack_forget() + update_scrollregion() + return + + for key, chk in checkbox_widgets.items(): + if regex.search(key): + chk.pack(anchor="w") + else: + chk.pack_forget() + + filter_list() + update_scrollregion() + + filter_var.trace_add("write", filter_list) + + # --- select / deselect buttons --- + button_frame = ttk.Frame(container) + button_frame.grid(row=2, column=0, columnspan=2, sticky="w", pady=(4, 0)) + + def select_visible(state: bool): + for key, chk in checkbox_widgets.items(): + if chk.winfo_manager(): # only visible (i.e., packed) widgets + vars_by_key[key].set(state) + + ttk.Button( + button_frame, + text="Select all", + command=lambda: select_visible(True), + width=12, + ).pack(side="left", padx=(0, 4)) + + ttk.Button( + button_frame, + text="Deselect all", + command=lambda: select_visible(False), + width=12, + ).pack(side="left") + + container.selection_vars = vars_by_key + return container + + +class ReferenceWidgetcreator: + _reference_options: list[str] + + def __init__(self, references: dict | None = None, reference_path: Traversable | None = None): + if references is None and reference_path is None: + return + if references is not None and reference_path is not None: + raise ValueError('Both references and reference_file supplied to ReferenceWidgetcreator.') + elif references is not None: + self.references = references + self.reference_path = None + else: + self.load_references_from_json(reference_path) + + # ---------- file helpers ---------- + def load_references_from_json(self, reference_path: Traversable): + self.reference_path = reference_path + with open(reference_path, "r", encoding="utf-8") as f: + self.references = json.load(f) + + def _save_references(self, data: dict): + with open(self.reference_path, "w", encoding="utf-8") as f: + json.dump(data, f, indent=4) + + @property + def reference_options(self): + return self._reference_options + + @reference_options.getter + def reference_options(self): + return sorted(self.references) + + # Main widget! + def create_widget(self, frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + combo = ttk.Combobox( + container, + width=40, + state="normal", + values=self.reference_options + ) + combo.grid(row=0, column=0, pady=4) + + def filter_references(_): + typed = combo.get().lower() + filtered = [ + key for key in self.reference_options + if typed in key.lower() + ] + combo["values"] = filtered + + combo.bind("", filter_references) + + def auto_complete(_): + typed = combo.get().lower() + filtered = [name for name in self.reference_options if typed in name.lower()] + if filtered: + combo.set(filtered[0]) + + combo.bind("", auto_complete) + + add_new = ttk.Button( + container, + text="New Ref", + command=lambda: self._open_new_reference_form(combo) + ) + add_new.grid(row=0, column=1, padx=(6, 0)) + + return combo + + def _open_new_reference_form(self, combo: ttk.Combobox): + win = tk.Toplevel() + win.title("Add New Reference") + win.transient() + win.grab_set() + + fields = [ + ("Title", "title"), + ("Authors (one per line)", "author"), + ("Year", "year"), + ("Month", "month"), + ("Journal", "journal"), + ("Volume", "volume"), + ("Pages", "pages"), + ("URL", "url"), + ("DOI", "doi"), + ] + + entries = OrderedDict() + + long_entries = {'Title', 'Authors (one per line)'} + + for row, (label, key) in enumerate(fields): + ttk.Label(win, text=label).grid(row=row, column=0, sticky="w", pady=4, padx=4) + if label not in long_entries: + entry = tk.Entry(win, width=50) + else: + entry = scrolledtext.ScrolledText(win, width=50, height=3) + + def focus_next_widget(event): + event.widget.tk_focusNext().focus() + return "break" + + entry.bind("", focus_next_widget) + + entry.grid(row=row, column=1, pady=4, padx=4) + entries[key] = entry + + # ---------- submit logic ---------- + def submit(): + try: + authors = [ + a.strip() + for a in entries["author"].get("1.0", 'end-1c').splitlines() + if a.strip() + ] + if not authors: + raise ValueError("At least one author is required") + + year = entries["year"].get().strip() + if not year: + raise ValueError("Year is required") + + title = entries['title'].get("1.0", 'end-1c') + citation_key = authors[0].split()[-1].lower() + '_' + title.lower().split()[0] + '_' + year + + references = self.references + if citation_key in references: + raise ValueError(f"Reference '{citation_key}' already exists") + + references[citation_key] = { + "title": title, + "author": authors, + "year": year, + "month": entries["month"].get() or None, + "journal": entries["journal"].get() or None, + "volume": entries["volume"].get(), + "pages": entries["pages"].get(), + "url": entries["url"].get() or None, + "doi": entries["doi"].get() or None, + } + + self._save_references(references) + + # update combobox + combo["values"] = self.reference_options + combo.set(citation_key) + + win.destroy() + + except ValueError as e: + messagebox.showerror("Invalid Reference", str(e), parent=win) + + ttk.Button(win, text="Submit", command=submit).grid( + row=len(fields), column=0, columnspan=2, pady=10 + ) + + @staticmethod + def _parse_int(value: str): + value = value.strip() + return int(value) if value else None + + +class SelectWidgetCreator: + def __init__(self, options: list[str]): + if not options: + raise ValueError("SelectWidgetCreator requires a non-empty options list") + self.options = options + + def create_widget(self, frame, row) -> tk.Widget: + combo = ttk.Combobox( + frame, + values=self.options, + state="readonly", + width=40 + ) + combo.grid(row=row, column=1, pady=4, sticky="w") + + # auto-select first option + combo.current(0) + + return combo + + +class TransitionWidgetCreator: + + @staticmethod + def create_widget(frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + upper_entry = ttk.Entry(container, width=18) + lower_entry = ttk.Entry(container, width=18) + + upper_entry.grid(row=0, column=0, padx=(0, 5)) + ttk.Label(container, text="→").grid(row=0, column=1) + lower_entry.grid(row=0, column=2, padx=(5, 0)) + + # Attach for processor access + container.upper_entry = upper_entry + container.lower_entry = lower_entry + + return container + + +class MultiTransitionWidgetCreator: + + @staticmethod + def create_widget(frame, row): + + class MultiContainer(ttk.Frame): # Mainly for type hinting + def __init__(self, transition_entries, buttons, *args, **kwargs): + super().__init__(frame, *args, **kwargs) + self.transition_entries: list[tuple[tk.Label, tk.Frame]] = transition_entries + self.buttons: list[tk.Button] = buttons + + def regrid(self): + for i, (label, transition_frame) in enumerate(self.transition_entries): + label.grid(row=i), transition_frame.grid(row=i) + for button in self.buttons: + button.grid(row=len(self.transition_entries)) + + container = MultiContainer(transition_entries=[], buttons=[]) + container.grid(row=row, column=1, pady=4, sticky="w") + + def add_new_transition(*_): + number_of_rows = len(container.transition_entries) + new_letter = f'{chr(ord("A") + number_of_rows)}' + + label = tk.Label(container, text=f'{new_letter}') + label.grid(row=number_of_rows, column=0) + + transition_frame = ttk.Frame(container) # Contains label and transition_frame + transition_frame.grid(row=number_of_rows, column=1) + + upper_entry = ttk.Entry(transition_frame, width=18) + lower_entry = ttk.Entry(transition_frame, width=18) + + upper_entry.grid(row=0, column=0, padx=(0, 5)) + ttk.Label(transition_frame, text="→").grid(row=0, column=1) + lower_entry.grid(row=0, column=2, padx=(5, 0)) + + transition_frame.upper_entry = upper_entry + transition_frame.lower_entry = lower_entry + + container.transition_entries.append((label, transition_frame)) + container.regrid() + + def delete_transition(*_): + label, transition_frame = container.transition_entries.pop() + label.grid_forget(), transition_frame.grid_forget() + container.regrid() + + add_button = ttk.Button(container, text="Add", command=add_new_transition, takefocus=0) + add_button.grid(row=0, column=0, pady=10) + + delete_button = ttk.Button(container, text="Remove", command=delete_transition, takefocus=0) + delete_button.grid(row=0, column=1, pady=10) + container.buttons = [add_button, delete_button] + add_new_transition(), add_new_transition() + + return container + + +class FieldSpec(NamedTuple): + name: str + processor: FieldProcessor + widget_creator: Widgetcreator = DefaultWidgetcreator() + hovertext: str | None = None + + +class InputTemplate(NamedTuple): + name: str + fields: list[FieldSpec] + data_key: Callable[[dict[str, Any]], str] + + +# Useful fields that get reused +reference_field = FieldSpec("Reference", ReferenceProcessor(reference_path=config['reference_path']), + ReferenceWidgetcreator(reference_path=config['reference_path'])) + +nuclide_field = FieldSpec("Nuclide", NuclideProcessor(), hovertext='Provide a nuclide in the format Pb208') + +transition_field = FieldSpec("Transition", TransitionProcessor(), TransitionWidgetCreator(), + hovertext='Enter the upper and lower levels of the atomic/muonic transition') + +notes_field = FieldSpec("Notes", CastProcessor(str, allows_empty=True)) + +# LIST TEMPLATES HERE. Each template must include a FieldSpec named "Reference". +muonic_transition_energy_template = InputTemplate( + name="Muonic Transition Energy", + fields=[ + reference_field, + nuclide_field, + transition_field, + FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'muonic', values['Nuclide'], + values['Transition']['Upper'], values['Transition']['Lower']])) + +muonic_transition_energy_difference_template = InputTemplate( + name="Muonic Transition Energy Difference (different nuclides)", + fields=[ + reference_field, + FieldSpec("Nuclide A", NuclideProcessor()), + FieldSpec("Nuclide B", NuclideProcessor()), + transition_field, + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'muonic_difference', values['NuclideA'], values['NuclideB'], + values['Transition']['Upper'], values['Transition']['Lower']]) +) + +muonic_transition_energy_difference_diff_transition_template = InputTemplate( + name="Muonic Transition Energy Difference (different transitions)", + fields=[ + reference_field, + nuclide_field, + FieldSpec("Transitions", MultiTransitionProcessor(), MultiTransitionWidgetCreator(), + hovertext='Enter the upper and lower levels of the atomic/muonic transition'), + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'muonic_difference', values['Nuclide'], + *list(sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values['Transitions'].items()], ()))]) +) + +muonic_barret_theory_template = InputTemplate( + name="Muonic Barrett Moment", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + FieldSpec('Rka [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('k [-]', CastProcessor(str)), + FieldSpec('alpha [1/fm]', CastProcessor(str)), + FieldSpec('Cz [fm/keV]', CastProcessor(str)), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'barrett_moment', values['Nuclide'], + *['-'.join(s.split('_')[-2:]) for s in + values['Previous Muonic Measurements']]]) +) + +muonic_radius_template = InputTemplate( + name="Muonic Radius", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + FieldSpec('R [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('Nuclear Polarization Method', SelectProcessor(['Calculated', 'Fit']), + SelectWidgetCreator(['Calculated', 'Fit']), + hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), + FieldSpec('Reduced Chi-Squared', CastProcessor(float, allows_empty=True)), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'radius', values['Nuclide'], + 'NP', values['Nuclear Polarization Method']]) +) + +muonic_fermi_distribution_template = InputTemplate( + name="Fermi Distribution", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + # TODO add fermi distribution processor and widget creator with different fermi distribution options. + FieldSpec('c [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('a [fm]', NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'fermi', values['Nuclide']]) +) + +templates = [muonic_transition_energy_template, + muonic_transition_energy_difference_template, + muonic_transition_energy_difference_diff_transition_template, + muonic_barret_theory_template, + muonic_radius_template, + muonic_fermi_distribution_template] + + +class DataEntryInterface: + templates: list[InputTemplate] + current_entries: OrderedDict[str, tuple[tk.Widget, FieldProcessor]] + references: dict[str, Reference] + reference_path: Traversable | None + compilation_folder: Traversable + + def __init__(self, + references: dict[str, Reference] | Traversable | None = None, + compilation_folder: Optional[str | Traversable] = None): + + self.root = tk.Tk() + self.root.title("Data Entry Interface") + + def _on_mousewheel(event): + widget = event.widget + try: + widget.yview_scroll(int(-1 * (event.delta / 120)), "units") + except AttributeError: + pass + + self.root.bind_all("", _on_mousewheel) + + if references is None: + self._load_references_from_json(config['reference_path']) + elif isinstance(references, Traversable): + self._load_references_from_json(references) + elif isinstance(references, dict): + self.reference_path = None + self.references = references + + compilation_folder = compilation_folder if compilation_folder is not None else config['compilation_dir'] + self.compilation_folder = Path(compilation_folder) if not isinstance(compilation_folder, + Traversable) else compilation_folder + + # Register templates here + self.templates = templates + + self.last_submitted = tk.StringVar() + self.field_widgets = {} # field_name -> widget + self.keep_vars = {} # field_name -> BooleanVar + + self.current_entries: OrderedDict[ + str, tuple[tk.Widget, FieldProcessor]] = OrderedDict() # Stores tk entry objects for each field displayed. + self.show_template_selection() + + def _load_references_from_json(self, reference_path: Optional[str | Traversable] = None): + with open(reference_path, "r", encoding="utf-8") as f: + raw_refs = json.load(f) + + self.reference_path = reference_path + self.references = {key: Reference(**value) for key, value in raw_refs.items()} + + def clear_window(self): + for widget in self.root.winfo_children(): + widget.destroy() + + def show_template_selection(self): + self.clear_window() + + ttk.Label( + self.root, + text="Select Data Entry Template", + font=("Arial", 16, "bold") + ).pack(pady=10) + + self.template_var = tk.StringVar() + + names = [t.name for t in self.templates] + + template_combo = ttk.Combobox( + self.root, + textvariable=self.template_var, + values=names, + font=("Arial", 12), + state="readonly", + width=60 + ) + template_combo.pack(pady=5) + + ttk.Button( + self.root, + text="Continue", + command=self.load_selected_template + ).pack(pady=10) + + def load_selected_template(self): + selected_name = self.template_var.get() + if not selected_name: + messagebox.showerror("Error", "Please select a template.") + return + + for template in self.templates: + if template.name == selected_name: + self.display_input(template) + return + + def display_input(self, template: InputTemplate): + self.clear_window() + self.current_entries.clear() + + ttk.Label( + self.root, + text=template.name, + font=("Arial", 16, "bold"), + wraplength=300 + ).pack(pady=10) + + form_frame = ttk.Frame(self.root) + form_frame.pack(padx=10, pady=10, fill="x") + + for row, field in enumerate(template.fields): + label = ttk.Label(form_frame, + text=field.name, + font=("Arial", 11), + wraplength=120 + ) + label.grid(row=row, column=0, sticky='w', pady=4) + if field.hovertext: + ToolTip(label, field.hovertext) + + entry = field.widget_creator.create_widget(form_frame, row) + self.current_entries[field.name] = (entry, field.processor) + + keep_var = tk.BooleanVar(value=False) + self.keep_vars[field.name] = keep_var + + keep_check = ttk.Checkbutton( + form_frame, + text="Keep", + variable=keep_var, + takefocus=0 + ) + keep_check.grid(row=row, column=2, padx=(6, 0)) + + button_frame = ttk.Frame(self.root) + button_frame.pack(pady=10) + + submit = ttk.Button( + button_frame, + text="Submit", + command=lambda: self.submit_data(template) + ) + submit.grid(row=0, column=0, padx=5) + submit.bind("", lambda _: self.submit_data(template)) + + ttk.Button( + button_frame, + text="Back", + command=self.show_template_selection + ).grid(row=0, column=1, padx=5) + + ttk.Button( + button_frame, + text="2D", + command=lambda: self.select_for_twod_input(template) + ).grid(row=0, column=2, padx=5) + + ttk.Label( + button_frame, + textvariable=self.last_submitted, + font=("Arial", 10) + ).grid(row=1, column=0, pady=3) + + def select_for_twod_input(self, template): + dialog = tk.Toplevel(self.root) + dialog.title("2D Input Selection") + dialog.transient(self.root) + dialog.grab_set() + + ttk.Label( + dialog, + text="Select the fields you would like to form the row index, column index, and the value you want to enter " + "for each row/column pair.", + wraplength=400, + justify="left" + ).pack(padx=20, pady=15) + + field_names = [field.name for field in template.fields] + btn_frame = ttk.Frame(dialog) + btn_frame.pack(fill="both", expand=True, padx=20, pady=10) + buttons = [] + + for i, selection in enumerate(['Row Field', 'Column Field', 'Value Field']): + tk.Label(btn_frame, text=selection).grid(row=i, column=0) + button = SelectWidgetCreator(field_names).create_widget(btn_frame, row=i) + buttons.append(button) + + def create_2d(): + field_answers = [btn.get() for btn in buttons] + dialog.destroy() + self.twod_input(template, *field_answers) + + ttk.Button(btn_frame, text="Create 2D", + command=create_2d).grid(row=3, column=0, padx=5) + ttk.Button(btn_frame, text="Back", command=lambda: dialog.destroy()).grid(row=3, column=1, padx=5) + + self.root.wait_window(dialog) + + def twod_input(self, template, row_field, col_field, value_field): + dialog = tk.Toplevel(self.root) + dialog.title(f"2D Input Selection: Values={value_field}") + dialog.transient(self.root) + dialog.grab_set() + + frame = ttk.Frame(dialog) + frame.pack(fill="both", expand=True, padx=10, pady=10) + + ttk.Label(frame, text=row_field).grid(row=1, column=0, padx=5, pady=5) + ttk.Label(frame, text=col_field).grid(row=0, column=1, padx=5, pady=5) + + grid_frame = ttk.Frame(frame) + grid_frame.grid(row=1, column=1) + + row_btn_frame = ttk.Frame(frame) + row_btn_frame.grid(row=2, column=0, sticky="n") + ttk.Button(row_btn_frame, text="+", command=lambda: grow_grid(rows=1, columns=0)).pack() + ttk.Button(row_btn_frame, text="-", command=lambda: shrink_grid(rows=1, columns=0)).pack() + + col_btn_frame = ttk.Frame(frame) + col_btn_frame.grid(row=0, column=2, sticky="e") + ttk.Button(col_btn_frame, text="+", command=lambda: grow_grid(rows=0, columns=1)).pack(side="left") + ttk.Button(col_btn_frame, text="-", command=lambda: shrink_grid(rows=0, columns=1)).pack(side="left") + + main_btn_frame = ttk.Frame(frame) + main_btn_frame.grid(row=0, column=0, sticky='w') + tk.Button(main_btn_frame, text='Submit', + command=lambda: self.submit_2d(template, row_field, col_field, value_field, row_widgets, col_widgets, cells)).pack() + tk.Button(main_btn_frame, text='Back', command=lambda: dialog.destroy()).pack() + + row_widgets: list[tk.Widget] = [] + col_widgets: list[tk.Widget] = [] + cells: list[list[tk.Widget]] = [] + + def make_widget(field_name): + field, = [field for field in template.fields if field.name == field_name] + return field.widget_creator.create_widget(grid_frame, row=0) + + def regrid(): + for w in grid_frame.winfo_children(): + w.grid_forget() + + # Column headers + for j, cw in enumerate(col_widgets): + cw.grid(row=0, column=j + 1, padx=5, pady=5, sticky="nsew") + grid_frame.columnconfigure(j + 1, weight=1) + + # Row headers + cells + for i, rw in enumerate(row_widgets): + rw.grid(row=i + 1, column=0, padx=5, pady=5, sticky="nsew") + grid_frame.rowconfigure(i + 1, weight=1) + + for j, cell in enumerate(cells[i]): + cell.grid(row=i + 1, column=j + 1, padx=5, pady=5, sticky="nsew") + cell.bind("", lambda e, fi=i, fj=j: (cells[fi][(fj + 1) % len(cells[fi])].focus(), "break")[1]) + cell.bind("", lambda e, fi=i, fj=j: (cells[(fi + 1) % len(cells)][fj].focus(), "break")[1]) + + def grow_grid(rows, columns): + if rows: + rw = make_widget(row_field) + rw.config(takefocus=0) + row_widgets.append(rw) + + new_row = [make_widget(value_field) for _ in col_widgets] + cells.append(new_row) + + if columns: + cw = make_widget(col_field) + cw.config(takefocus=0) + col_widgets.append(cw) + + for row in cells: + row.append(make_widget(value_field)) + + regrid() + + def shrink_grid(rows, columns): + if rows and row_widgets: + row_widgets.pop().destroy() + for cell in cells.pop(): + cell.destroy() + + if columns and col_widgets: + col_widgets.pop().destroy() + for row in cells: + row.pop().destroy() + + regrid() + + grow_grid(rows=2, columns=2) + + def submit_2d(self, template, row_field, col_field, value_field, row_widgets, col_widgets, cells): + # We take each (row_widget, col_widget, cell_widget) triplet, fill them in to the main data entry tab, + # and trigger the data submission. + + original_entries = {field_name: self.current_entries[field_name] for field_name in (row_field, col_field, value_field)} + + for row_widget, cell_row in zip(row_widgets, cells): + for col_widget, cell in zip(col_widgets, cell_row): + for field_name, widget in [(row_field, row_widget), (col_field, col_widget), (value_field, cell)]: + prev_entry, processor = self.current_entries[field_name] + self.current_entries[field_name] = (widget, processor) + self.submit_data(template, clear_fields=False) # We don't want to erase our row/col entries as we submit + + for field_name in (row_field, col_field, value_field): # make sure we restore the original widgets once we are done submitting. + self.current_entries[field_name] = original_entries[field_name] + + pass + + def submit_data(self, template: InputTemplate, clear_fields=True): + + def clear_widget(widg: tk.Widget): + if isinstance(widg, ttk.Entry): + widg.delete(0, tk.END) + return + + # Composite widgets (e.g. Transition frame) + for child in widget.winfo_children(): + if isinstance(child, ttk.Entry): + child.delete(0, tk.END) + + data = OrderedDict() + + try: + for field_name, (widget, processor) in self.current_entries.items(): + data[field_name] = processor.process(widget) + except ValueError as e: + messagebox.showerror("Invalid Input", str(e)) + return + + self.save_data(template, data) + + focus_widget = None + for field_name, (widget, _) in self.current_entries.items(): + if not self.keep_vars[field_name].get() and clear_fields: + clear_widget(widget) + if focus_widget is None: + widget.focus() + focus_widget = widget + + self.last_submitted.set(f'Last Submitted: {template.data_key(data)}') + + def save_data( + self, + template: InputTemplate, + data: dict, + replacement_strategy: Literal["Ask", "AlwaysReplace", "NeverReplace"] = "Ask", + ) -> None: + + data_key = template.data_key(data) + file_dir = self.compilation_folder / data["Reference"] + file_dir.mkdir(parents=True, exist_ok=True) + + file = file_dir / f"{template.name}.json" + + new_entry = {data_key: data} + + if file.exists(): + with file.open("r", encoding="utf-8") as f: + existing_data = json.load(f) + + if data_key in existing_data: + match replacement_strategy: + case "AlwaysReplace": + existing_data[data_key] = data + + case "NeverReplace": + return + + case "Ask": + action = self._ask_collision_action(self.root, data_key, file) + + if action == "replace": + existing_data[data_key] = data + + elif action == "suffix": + new_key = self._next_available_key(data_key, existing_data) + existing_data[new_key] = data + + else: # do nothing + return + else: + existing_data[data_key] = data + + data_to_write = existing_data + + else: + data_to_write = new_entry + + with file.open("w", encoding="utf-8") as f: + json.dump(data_to_write, f, indent=4) + + print(f"Data successfully saved to {file}") + + @staticmethod + def _next_available_key(base_key: str, existing: dict) -> str: + suffix = ord("a") + while True: + candidate = f"{base_key}_{chr(suffix)}" + if candidate not in existing: + return candidate + suffix += 1 + + @staticmethod + def _ask_collision_action(parent, key: str, file: Path) -> str | None: + """ + Returns: 'replace', 'suffix', or None (do nothing) + """ + result = None + dialog = tk.Toplevel(parent) + dialog.title("Duplicate Entry") + dialog.transient(parent) + dialog.grab_set() + + ttk.Label( + dialog, + text=f"'{key}' already exists in:\n{file}\n\nWhat would you like to do?", + wraplength=400, + justify="left" + ).pack(padx=20, pady=15) + + def choose(action): + nonlocal result + result = action + dialog.destroy() + + btns = ttk.Frame(dialog) + btns.pack(pady=10) + + ttk.Button(btns, text="Replace", command=lambda: choose("replace")).grid(row=0, column=0, padx=5) + ttk.Button(btns, text="Add Suffix", command=lambda: choose("suffix")).grid(row=0, column=1, padx=5) + ttk.Button(btns, text="Do Nothing", command=lambda: choose(None)).grid(row=0, column=2, padx=5) + + parent.wait_window(dialog) + return result + + +if __name__ == "__main__": + interface = DataEntryInterface(references=config['reference_path']) + interface.root.mainloop() diff --git a/radbase/radius_analyzer.py b/radbase/radius_analyzer.py index 46273b6..4439492 100644 --- a/radbase/radius_analyzer.py +++ b/radbase/radius_analyzer.py @@ -13,40 +13,7 @@ from lmfit import Minimizer, Parameters from uncertainties import correlated_values_norm, correlation_matrix, ufloat -from .converter import Measurement - - -class Nuclide: - z: int - a: int - - def __init__(self, nucstr): - self.nucstr = nucstr - nucstr = nucstr[1:] - self.z = int(nucstr[:3]) - self.a = int(nucstr[3:]) - self.n = self.a - self.z - - def guess_radius(self): - # semiempirical estimate - return (0.9071 + 1.1025 / (self.a ** (2 / 3)) + -0.548 / (self.a ** (4 / 3))) * self.a ** (1 / 3) - - def __repr__(self): - return f'Nuclide (Z={self.z}, A={self.a})' - - def __eq__(self, other): - return (self.z == other.z) and (self.a == other.a) - - def __lt__(self, other): - if self.z != other.z: - return self.z < other.z - return self.a < other.a - - def __hash__(self): - return self.z * 1000 + self.a - - def __str__(self): - return f'R{self.z:03}{self.a:03}' +from .converter import Measurement, Nuclide class Term: diff --git a/tests/test_converter.py b/tests/test_converter.py new file mode 100644 index 0000000..b3f6d02 --- /dev/null +++ b/tests/test_converter.py @@ -0,0 +1,4 @@ + +from uncertainties import ufloat + +from radbase.converter import Quantity, QuantityType diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py new file mode 100644 index 0000000..eec6229 --- /dev/null +++ b/tests/test_data_entry.py @@ -0,0 +1,150 @@ +import json +import pathlib +import tkinter as tk +from tkinter import ttk + +import pytest + +from radbase.data_entry import (CastProcessor, DataEntryInterface, FieldSpec, + InputTemplate, NuclideProcessor, + NumberWithUncertaintyProcessor, + ReferenceProcessor, templates) + +example_references = { + "Smith_nuclear_1978": { + "title": "Nuclear Charge Radii from Muonic Atoms", + "author": ["John Smith", "Alice Jones"], + "year": "1978", + }, + "Brown_isotope_1992": { + "title": "Isotope Shifts in Heavy Nuclei", + "author": ["Michael Brown"], + "year": "1992" + } +} + +# Maps field names in data_entry.templates to example outputs. +example_outputs = { + 'Reference': list(example_references.keys())[0], + 'Previous Muonic Measurements': list(example_references.keys())[0] + '_muonic_2p1/2_1s1/2', + 'Nuclide': 'Pb208' + '' + + +} + + +def make_dummy_references(tmp_path): + temp_references_file = tmp_path / 'references.json' + temp_references_file.write_text(json.dumps(example_references)) + return temp_references_file + + +class DummyProcessor: + @staticmethod + def process(widget): + return 'nothing' + + +dummy_template = InputTemplate(name='test', + fields=[FieldSpec('Reference', CastProcessor(str)), + FieldSpec('testfield', DummyProcessor())], + data_key=lambda x: 'testkey') + + +class DummyWidget(ttk.Widget): + def __init__(self, value): + self.value = value + + def get(self): + return self.value + + +def test_cast_processor(): + widget = DummyWidget('30.2') + blank_widget = DummyWidget('') + + assert CastProcessor(str).process(widget) == '30.2' + assert CastProcessor(float).process(widget) == 30.2 + + with pytest.raises(ValueError) as e_info: # should raise error if it can not cast + CastProcessor(int).process(widget) + with pytest.raises(ValueError) as e_info: # should raise error if field was left blank. + CastProcessor(str).process(blank_widget) + + +def test_nuclide_processor(): + widget = DummyWidget('Pb208') + natwidget = DummyWidget('Pbnat') + bad_widget = DummyWidget('082203') + + assert NuclideProcessor().process(widget) == 'Pb208' + assert NuclideProcessor().process(natwidget) == 'Pbnat' + with pytest.raises(ValueError) as e_info: + NuclideProcessor().process(bad_widget) + + +def test_reference_processor(tmp_path): + + global example_references + + good_widget = DummyWidget('Smith_nuclear_1978') + bad_widget = DummyWidget('Noone_title_1340') + + tmp_ref_path = make_dummy_references(tmp_path) + ref_proc = ReferenceProcessor(tmp_ref_path) + + assert ref_proc.process(good_widget) == 'Smith_nuclear_1978' + with pytest.raises(ValueError) as e_info: + ref_proc.process(bad_widget) + + +def test_number_with_uncertainty_processor(): + + float_widget = DummyWidget('100.1') + uncertainty_widget = DummyWidget('100.1(3)') + bad_widget = DummyWidget('bad') + + ref_proc = NumberWithUncertaintyProcessor() + + assert ref_proc.process(float_widget) == {'value': 100.1, 'uncertainty': None} + assert ref_proc.process(uncertainty_widget) == {'value': 100.1, 'uncertainty': 0.3} + with pytest.raises(ValueError) as e_info: + ref_proc.process(bad_widget) + + +def test_init_data_entry_interface(tmp_path): + + global example_references + + temp_references_file = tmp_path / 'references.json' + temp_references_file.write_text(json.dumps(example_references)) + + DataEntryInterface() + + +def test_save_data(tmp_path): + + ref_key = list(example_references.keys())[0] + test_data = {'Reference': ref_key, 'testfield': 3} + tmp_path.mkdir(exist_ok=True) + tmp_data_loc = tmp_path / ref_key / f'{dummy_template.name}.json' + + interface = DataEntryInterface(compilation_folder=tmp_path) + + interface.save_data(dummy_template, test_data, replacement_strategy='AlwaysReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': test_data} + + new_test_data = test_data.copy() + new_test_data['testfield'] = 5 + interface.save_data(dummy_template, new_test_data, replacement_strategy='AlwaysReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': new_test_data} + + interface.save_data(dummy_template, test_data, replacement_strategy='NeverReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': new_test_data} + + +# def test_previous_measurement_processor(tmp_path): +# +# previous_measurements = {'Authors'} +# proc = PreviousMeasurementProcessor(previous_measurements = {}) From 4d286a265a46b25d1f28c169afa7ed0e882c926e Mon Sep 17 00:00:00 2001 From: Hunter Date: Sat, 31 Jan 2026 15:35:03 -0500 Subject: [PATCH 03/11] Added DataEntryInterface and template systems. Entered Ke75 and Be88. --- .github/workflows/python-package-testing.yml | 2 +- .pre-commit-config.yaml | 1 + .../Muonic Barrett Moment.json | 110 ++ .../bergem_nuclear_1988/Muonic Radius.json | 46 + .../Muonic Transition Energy.json | 182 +++ .../compilation/bergem_nuclear_1988/notes.txt | 1 + .../Fermi Distribution.json | 126 ++ .../kessler_muonic_1975/Muonic Radius.json | 58 + ...gy Difference (different transitions).json | 658 +++++++++ .../Muonic Transition Energy.json | 834 ++++++++++++ radbase/compilation/references.json | 70 + .../Muonic Transition Energy.json | 110 ++ radbase/converter.py | 141 +- radbase/data_entry.py | 1203 +++++++++++++++++ radbase/radius_analyzer.py | 35 +- tests/test_converter.py | 4 + tests/test_data_entry.py | 156 +++ 17 files changed, 3691 insertions(+), 46 deletions(-) create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Radius.json create mode 100644 radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json create mode 100644 radbase/compilation/bergem_nuclear_1988/notes.txt create mode 100644 radbase/compilation/kessler_muonic_1975/Fermi Distribution.json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Radius.json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json create mode 100644 radbase/compilation/kessler_muonic_1975/Muonic Transition Energy.json create mode 100644 radbase/compilation/references.json create mode 100644 radbase/compilation/test_test_1700/Muonic Transition Energy.json create mode 100644 radbase/data_entry.py create mode 100644 tests/test_converter.py create mode 100644 tests/test_data_entry.py diff --git a/.github/workflows/python-package-testing.yml b/.github/workflows/python-package-testing.yml index fcf2a6b..76feaef 100644 --- a/.github/workflows/python-package-testing.yml +++ b/.github/workflows/python-package-testing.yml @@ -8,7 +8,7 @@ jobs: runs-on: ubuntu-latest strategy: matrix: - python-version: ["3.11", "3.12", "3.13"] + python-version: ["3.12", "3.13"] steps: - uses: actions/checkout@v3 diff --git a/.pre-commit-config.yaml b/.pre-commit-config.yaml index 4ab80ef..4a1baf6 100644 --- a/.pre-commit-config.yaml +++ b/.pre-commit-config.yaml @@ -19,6 +19,7 @@ repos: hooks: - id: flake8 additional_dependencies: [flake8-deprecated, flake8-mutable, Flake8-pyproject] + exclude: tests/ - repo: https://github.com/PyCQA/isort/ rev: 5.13.2 diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json b/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json new file mode 100644 index 0000000..0699bf7 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Barrett Moment.json @@ -0,0 +1,110 @@ +{ + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.8821(6)", + "k [-]": "1.1456", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "-2.136E-5", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9370(3)", + "k [-]": "1.3993", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "-1.268E-5", + "Notes": "" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9960(3)", + "k [-]": "1.8474", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "8.547E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "6.9958(4)", + "k [-]": "1.8715", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "7.909E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.0319(1)", + "k [-]": "2.2429", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.478E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.0320(1)", + "k [-]": "2.2559", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.406E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1222(3)", + "k [-]": "3.4781", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "9.128E-6", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1654(9)", + "k [-]": "4.0454", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.329E-5", + "Notes": "Experimental Uncertainty Only" + }, + "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2" + ], + "Nuclide": "Pb208", + "Rka [fm]": "7.1670(4)", + "k [-]": "4.0699", + "alpha [1/fm]": "0.1415", + "Cz [fm/keV]": "1.318E-5", + "Notes": "Experimental Uncertainty Only" + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json b/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json new file mode 100644 index 0000000..4e3796a --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Radius.json @@ -0,0 +1,46 @@ +{ + "bergem_nuclear_1988_radius_Pb208_NP_Calculated": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.504, + "uncertainty": 0.0011 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 187.0, + "Notes": "Fixed alpha=0.1415 from e- scattering" + }, + "bergem_nuclear_1988_radius_Pb208_NP_Fit": { + "Reference": "bergem_nuclear_1988", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.5031, + "uncertainty": 0.0011 + }, + "Nuclear Polarization Method": "Fit", + "Reduced Chi-Squared": 0.19, + "Notes": "Alpha=0.1415, 2pf fit, " + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json b/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json new file mode 100644 index 0000000..e929040 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/Muonic Transition Energy.json @@ -0,0 +1,182 @@ +{ + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": "5962.854(90)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": "5778.058(100)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": "2642.332(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "2500.590(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "2457.569(70)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": "1507.754(50)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p1/2", + "Lower": "2s1/2" + }, + "Energy [keV]": "1460.558(32)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": "1215.330(30)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": "1030.543(27)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": "1404.659(20)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "1366.347(19)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "1361.748(250)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": "971.974(17)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "938.096(18)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d5/2" + }, + "Energy [keV]": "928.883(14)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d3/2", + "Lower": "3p1/2" + }, + "Energy [keV]": "920.959(28)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d5/2", + "Lower": "3p3/2" + }, + "Energy [keV]": "891.383(22)", + "Notes": "" + }, + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2": { + "Reference": "bergem_nuclear_1988", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4d3/2", + "Lower": "3p3/2" + }, + "Energy [keV]": "873.761(63)", + "Notes": "" + } +} diff --git a/radbase/compilation/bergem_nuclear_1988/notes.txt b/radbase/compilation/bergem_nuclear_1988/notes.txt new file mode 100644 index 0000000..cf57e62 --- /dev/null +++ b/radbase/compilation/bergem_nuclear_1988/notes.txt @@ -0,0 +1 @@ +TODO: Add the correlations between transition energies from Table VI diff --git a/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json b/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json new file mode 100644 index 0000000..b95e42c --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Fermi Distribution.json @@ -0,0 +1,126 @@ +{ + "kessler_muonic_1975_fermi_Pb208": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2" + ], + "Nuclide": "Pb208", + "c [fm]": { + "value": 6.65, + "uncertainty": 0.007 + }, + "a [fm]": { + "value": 0.526, + "uncertainty": 0.0014 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb207": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2" + ], + "Nuclide": "Pb207", + "c [fm]": { + "value": 6.647, + "uncertainty": 0.005 + }, + "a [fm]": { + "value": 0.523, + "uncertainty": 0.003 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb206": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2" + ], + "Nuclide": "Pb206", + "c [fm]": { + "value": 6.649, + "uncertainty": 0.019 + }, + "a [fm]": { + "value": 0.517, + "uncertainty": 0.01 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + }, + "kessler_muonic_1975_fermi_Pb204": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2" + ], + "Nuclide": "Pb204", + "c [fm]": { + "value": 6.627, + "uncertainty": 0.014 + }, + "a [fm]": { + "value": 0.52, + "uncertainty": 0.008 + }, + "Notes": "Fit done using 2p1/2, 2p3/2, 2s1/2, and 3p3/2 levels, but these levels determined from all transitions." + } +} diff --git a/radbase/compilation/kessler_muonic_1975/Muonic Radius.json b/radbase/compilation/kessler_muonic_1975/Muonic Radius.json new file mode 100644 index 0000000..be5870a --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Muonic Radius.json @@ -0,0 +1,58 @@ +{ + "kessler_muonic_1975_radius_Pb204_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb204" + ], + "Nuclide": "Pb204", + "R [fm]": { + "value": 5.4857, + "uncertainty": 0.0012 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.47, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb206_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb206" + ], + "Nuclide": "Pb206", + "R [fm]": { + "value": 5.497, + "uncertainty": 0.0015 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.73, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb208_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb208" + ], + "Nuclide": "Pb208", + "R [fm]": { + "value": 5.5097, + "uncertainty": 0.0006 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.11, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + }, + "kessler_muonic_1975_radius_Pb207_NP_Calculated": { + "Reference": "kessler_muonic_1975", + "Data used as input": [ + "kessler_muonic_1975_fermi_Pb207" + ], + "Nuclide": "Pb207", + "R [fm]": { + "value": 5.5036, + "uncertainty": 0.0004 + }, + "Nuclear Polarization Method": "Calculated", + "Reduced Chi-Squared": 0.05, + "Notes": "Oddly low chi-squared and error given the experimental/theoretical errorbars." + } +} diff --git a/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json b/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json new file mode 100644 index 0000000..bbd091c --- /dev/null +++ b/radbase/compilation/kessler_muonic_1975/Muonic Transition Energy Difference (different transitions).json @@ -0,0 +1,658 @@ +{ + "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 184.83, + "uncertainty": 0.01 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.09, + "uncertainty": 0.14 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 185.75, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "B": { + "Upper": "2p1/2", + "Lower": "1s1/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 186.04, + "uncertainty": 0.11 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 141.77, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 141.82, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "B": { + "Upper": "3d5/2", + "Lower": "2p3/2" + } + }, + "Energy Difference [keV] (A-B)": { + "value": 142.53, + "uncertainty": 0.05 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transitions": { + "A": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + 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"Nuclide": "Pb204", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2459.7, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2500.33, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2501.1, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2501.6, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2502.83, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2642.11, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2642.93, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2644.14, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2645.52, + "uncertainty": 0.07 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 937.98, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 937.83, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 937.87, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 937.99, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 971.85, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 971.83, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 971.86, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 971.86, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1366.52, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1366.42, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1366.4, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "5f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1366.57, + "uncertainty": 0.09 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1404.74, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1404.66, + "uncertainty": 0.08 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1404.62, + "uncertainty": 0.09 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "5f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1404.68, + "uncertainty": 0.11 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.67, + "uncertainty": 0.15 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.68, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.11, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "6f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 1599.8, + "uncertainty": 0.19 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1639.98, + "uncertainty": 0.19 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1640.23, + "uncertainty": 0.24 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1639.92, + "uncertainty": 0.24 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "6f5/2", + "Lower": "3d3/2" + }, + "Energy [keV]": { + "value": 1640.21, + "uncertainty": 0.34 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1030.44, + "uncertainty": 0.17 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1030.02, + "uncertainty": 0.27 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1029.99, + "uncertainty": 0.41 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1028.83, + "uncertainty": 0.38 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.43, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.6, + "uncertainty": 0.45 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1215.58, + "uncertainty": 0.54 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1214.12, + "uncertainty": 0.3 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb208", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1507.48, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb207", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1508.71, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1509.53, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2": { + "Reference": "kessler_muonic_1975", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3p3/2", + "Lower": "2s1/2" + }, + "Energy [keV]": { + "value": 1511.63, + "uncertainty": 0.2 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json new file mode 100644 index 0000000..a82f481 --- /dev/null +++ b/radbase/compilation/references.json @@ -0,0 +1,70 @@ +{ + "zehnder_charge_1975": { + "title": "CHARGE PARAMETERS, ISOTOPE SHIFTS, QUADRUPOLE MOMENTS, AND NUCLEAR EXCITATION IN MUONIC 170-174, 176yb", + "author": [ + "A. Zehnder", + "F. Boehm", + "W. Dey", + "R. Engfer", + "H. K. Walter", + "J. L. Vuilleumier" + ], + "year": "1975", + "month": null, + "journal": "Nuclear Physics A", + "volume": 254, + "pages": "315-340", + "url": "https://www.sciencedirect.com/science/article/abs/pii/0375947475902195", + "doi": "10.1016/0375-9474(75)90219-5" + }, + "bergem_nuclear_1988": { + "title": "Nuclear polarization and charge moments of \n208 Pb from muonic x rays", + "author": [ + "P. Bergem", + "G. Piller", + "A. Rueetschi", + "L. A. Schaller", + "L. Schellenberg", + "H. Schneuwly" + ], + "year": "1988", + "month": "June", + "journal": "Physical Review C", + "volume": "37", + "pages": "2821", + "url": "https://journals.aps.org/prc/abstract/10.1103/PhysRevC.37.2821", + "doi": "10.1103/PhysRevC.37.2821" + }, + "kessler_muonic_1975": { + "title": "Muonic x rays in lead isotopes", + "author": [ + "D. Kessler", + "H. Mes", + "A. C. Thompson", + "H. L. Anderson", + "M. S. Dixit", + "C. K. Hargrove", + "R. J. McKee" + ], + "year": "1975", + "month": "May", + "journal": "Physical Review C", + "volume": "11", + "pages": "1719-1734", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.11.1719", + "doi": "10.1103/PhysRevC.11.1719" + }, + "test_test_1700": { + "title": "Test", + "author": [ + "Test Test" + ], + "year": "1700", + "month": null, + "journal": null, + "volume": "", + "pages": "", + "url": null, + "doi": null + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy.json b/radbase/compilation/test_test_1700/Muonic Transition Energy.json new file mode 100644 index 0000000..f527937 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy.json @@ -0,0 +1,110 @@ +{ + "test_test_1700_muonic_Pb204_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb204", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 300.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb203_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb203", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 200.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb203_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb203", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 100.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb204_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb204", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 400.0, + "uncertainty": null + }, + "Composite?": "No", + "Notes": "" + }, + "test_test_1700_muonic_Pb200_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb200", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 202.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb200_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb200", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 203.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb100_2p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb100", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 102.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_Pb100_3p_1s": { + "Reference": "test_test_1700", + "Nuclide": "Pb100", + "Transition": { + "Upper": "3p", + "Lower": "1s" + }, + "Energy [keV]": { + "value": 103.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/converter.py b/radbase/converter.py index 4a0c9bd..3706aa0 100644 --- a/radbase/converter.py +++ b/radbase/converter.py @@ -1,32 +1,151 @@ -from abc import ABC +""" +Measurement -> ConvertedQuantity -> ... -> Radius -from .radius_analyzer import RadiiInformation +TODO: Consider better way of defining the type of a quantity. For example, each quantity will have a value and an +uncertainty, and then some kind of identifier (just a string?) for what those numbers go with. For now, I will use the +naive approach of using strings, although this will definitely come back to haunt me. +""" +from abc import ABC, abstractmethod +from dataclasses import dataclass, field +from typing import Callable, Literal, Tuple -class ConversionStep(ABC): - pass +from uncertainties import UFloat, ufloat +# from .radius_analyzer import Nuclide -class ConversionStrategy: - pass +# from .radius_analyzer import RadiiInformation -class ConversionRecord: +class Nuclide: + z: int + a: int - def __init__(self): - pass + def __init__(self, nucstr): + self.nucstr = nucstr + nucstr = nucstr[1:] + self.z = int(nucstr[:3]) + self.a = int(nucstr[3:]) + self.n = self.a - self.z + + def guess_radius(self): + # semiempirical estimate + return (0.9071 + 1.1025 / (self.a ** (2 / 3)) + -0.548 / (self.a ** (4 / 3))) * self.a ** (1 / 3) + + def __repr__(self): + return f'Nuclide (Z={self.z}, A={self.a})' + + def __eq__(self, other): + return (self.z == other.z) and (self.a == other.a) + + def __lt__(self, other): + if self.z != other.z: + return self.z < other.z + return self.a < other.a + + def __hash__(self): + return self.z * 1000 + self.a + def __str__(self): + return f'R{self.z:03}{self.a:03}' -class Measurement(ABC): + +class Transition: def __init__(self): + raise NotImplementedError() + + +class QuantityType(str): + pass + + +@dataclass +class Quantity: + uvar: UFloat + value: float = field(init=False) + unc: float = field(init=False) + unit: str + quantity: QuantityType + + def __post_init__(self): + self.value = self.uvar.n + self.unc = self.uvar.s + + +class MuonicTransitionEnergyMeasurement: + reference: str + transition: Transition + nuclide: Nuclide + uvar: UFloat + unit: Literal['eV'] + + +class OpticalIsotopeShiftMeasurement: + reference: str + transition: Transition + nuclide_heavier: Nuclide + nuclide_lighter: Nuclide + uvar: UFloat + unit: Literal['THz'] + + +@dataclass +class ConversionHistory: + + """Stores one step of how a converted quantity was obtained. Contains input quantites and ConverstionStep(s) followed + to reach the ConvertedQuantity. By following the chain of ConversionHistories, the full conversion process can + be reconstructed.""" + + conversion_text: str + input_quantities: Tuple[Quantity] + output_quantity: Quantity + conversion_func: Callable | None + + +@dataclass +class Measurement(Quantity): + ref: str | None + + +@dataclass +class ConvertedQuantity(Quantity): + history: ConversionHistory + + +class ConversionStep(ABC): + """ + Wrapper around a conversion function that indicates input data types, creates the conversion history for the output, + and returns the output type. + """ + + input_quantities: tuple[QuantityType] + output_quantity: QuantityType + conversion_function: Callable[[*Tuple[ufloat]], ufloat] # Variable number of ufloats as input, returns ufloat as output + + def __init__(self, input_quantities: tuple[QuantityType], output_quantity: QuantityType, + conversion_function: Callable[[*Tuple[ufloat]], ufloat]): + self.input_quantities = input_quantities + self.output_quantity = output_quantity + self.conversion_function = conversion_function + + @abstractmethod + def convert_quantity(self, *inputs) -> ConvertedQuantity: + pass + + @abstractmethod + def create_history(self, *inputs) -> ConversionHistory: pass +class ConversionStrategy: + pass + + class Converter: def __init__(self, conversion_strategy: ConversionStrategy): self.strategy = conversion_strategy - def convert(self, measurements: list[Measurement], conversion_steps) -> RadiiInformation: # or something like RI + def convert(self, measurements: list[Measurement], conversion_steps: list[Quantity]): # or something like RI pass diff --git a/radbase/data_entry.py b/radbase/data_entry.py new file mode 100644 index 0000000..48546e6 --- /dev/null +++ b/radbase/data_entry.py @@ -0,0 +1,1203 @@ +""" +A simple UI to assist with the compilation of previous nuclear radius information. +""" + +import json +import re +import tkinter as tk +from collections import OrderedDict +from dataclasses import dataclass +from importlib.resources import files +from importlib.resources.abc import Traversable +from pathlib import Path +from tkinter import messagebox, scrolledtext, ttk +from typing import Any, Callable, Literal, NamedTuple, Optional, Protocol + +import uncertainties + +config = { + 'compilation_dir': files('radbase') / 'compilation', + 'reference_path': files('radbase') / 'compilation/references.json' +} + + +@dataclass +class Reference: + title: str + author: list[str] + year: str + month: Optional[str] = None + journal: Optional[str] = None + pages: Optional[int] = None + volume: Optional[int] = None + url: Optional[str] = None + doi: Optional[str] = None + + +class ToolTip: + def __init__(self, widget, text: str, delay: int = 500): + self.widget = widget + self.text = text + self.delay = delay + self._after_id = None + self._tip = None + + widget.bind("", self._schedule) + widget.bind("", self._hide) + widget.bind("", self._hide) + + def _schedule(self, _): + self._after_id = self.widget.after(self.delay, self._show) + + def _show(self): + if self._tip or not self.text: + return + + x = self.widget.winfo_rootx() + 20 + y = self.widget.winfo_rooty() + self.widget.winfo_height() + 5 + + self._tip = tk.Toplevel(self.widget) + self._tip.wm_overrideredirect(True) + self._tip.wm_geometry(f"+{x}+{y}") + + label = ttk.Label( + self._tip, + text=self.text, + background="#ffffe0", + relief="solid", + borderwidth=1, + padding=6, + wraplength=300 + ) + label.pack() + + def _hide(self, _=None): + if self._after_id: + self.widget.after_cancel(self._after_id) + self._after_id = None + if self._tip: + self._tip.destroy() + self._tip = None + + +class FieldProcessor(Protocol): + def process(self, widget: tk.Widget) -> Any: + pass + + +class CastProcessor: + + def __init__(self, field_type: type, allows_empty: bool = False): + self.field_type = field_type + self.allows_empty = allows_empty + + def process(self, widget: tk.Widget): + raw = widget.get() + if raw == "" and not self.allows_empty: + raise ValueError("Field is empty") + return self.field_type(raw) + + +class NumberWithUncertaintyProcessor: + + @staticmethod + def process(widget: tk.Widget): + raw = widget.get().strip() + try: + value = float(raw) + return {'value': value, 'uncertainty': None} + except ValueError: + try: + uvar = uncertainties.ufloat_fromstr(raw) + return {'value': uvar.n, 'uncertainty': uvar.s} + except ValueError: + raise ValueError( + f'Entered value of {raw} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') + + +class MultiTransitionProcessor: + @staticmethod + def process(widget: tk.Widget): + data = {} + for label, container in widget.transition_entries: + data[label.cget("text")] = TransitionProcessor().process(container) + return data + + +class NuclideProcessor: + @staticmethod + def process(widget: tk.Widget): + raw = widget.get() + if re.match(r'[a-zA-Z]{2}\d{1,3}', raw): + return raw + elif re.match(r'[a-zA-Z]{2}nat', raw): + return raw + else: + raise ValueError( + 'Entered Nuclide does not match pattern of two letters and one to three numbers (Ex. Pb208') + + +class ReferenceProcessor: + def __init__(self, reference_path: Traversable): + self.reference_path = reference_path + + @property + def references(self): + pass + + @references.getter + def references(self): + with open(self.reference_path, 'r') as f: + return json.load(f) + + def process(self, widget: tk.Widget): + value = widget.get().strip() + + if value not in sorted(self.references.keys()): + raise ValueError( + f"Reference '{value}' is not a known citation key" + ) + + return value + + +class SelectProcessor: + def __init__(self, options: list[str]): + self.options = set(options) + + def process(self, widget: tk.Widget) -> str: + value = widget.get().strip() + + if not value: + raise ValueError("No option selected") + + if value not in self.options: + raise ValueError(f"'{value}' is not a valid selection") + + return value + + +class TransitionProcessor: + SIMPLE_LEVEL_PATTERN = re.compile( + r""" + ^ + \d+ # principal quantum number + [spdf] # orbital + (\d+/\d+)? # optional j (e.g. 3/2) + $ + """, + re.VERBOSE + ) + + HYBRID_LEVEL_PATTERN = re.compile( + r""" + ^ + \d+[+-] # nuclear spin/parity (e.g. 2+, 0-) + , + \d+ # principal quantum number + [spdf] # orbital + \d+/\d+ # required j + $ + """, + re.VERBOSE + ) + + def process(self, widget: tk.Widget) -> dict[str, str]: + upper = widget.upper_entry.get().strip() + lower = widget.lower_entry.get().strip() + + if not upper or not lower: + raise ValueError("Both upper and lower transition levels must be provided") + + upper_simple = self.SIMPLE_LEVEL_PATTERN.match(upper) + lower_simple = self.SIMPLE_LEVEL_PATTERN.match(lower) + + upper_hybrid = self.HYBRID_LEVEL_PATTERN.match(upper) + lower_hybrid = self.HYBRID_LEVEL_PATTERN.match(lower) + + # both simple or both hybrid + if upper_simple and lower_simple or upper_hybrid and lower_hybrid: + return {'Upper': upper, 'Lower': lower} + + raise ValueError( + "Invalid transition format.\n" + "Both levels must be either:\n" + " - Simple atomic levels (e.g. 2p3/2)\n" + " - Hybrid nuclear+atomic levels (e.g. 2+,1s1/2)" + ) + + +class PreviousMeasurementProcessor: + @staticmethod + def process(widget: tk.Widget) -> list[str]: + selected = [ + key + for key, var in widget.selection_vars.items() + if var.get() + ] + if not selected: + raise ValueError("At least one previous measurement must be selected") + return selected + + +class Widgetcreator(Protocol): + def create_widget(self, frame, row) -> tk.Widget: + pass + + +class DefaultWidgetcreator: + @staticmethod + def create_widget(frame, row) -> tk.Widget: + entry = ttk.Entry(frame, width=40) + entry.grid(row=row, column=1, pady=4, sticky='w') + return entry + + +class PreviousMeasurementWidgetCreator: + + def __init__(self, compilation_path: Traversable, filter_regex: str = ""): + self.filter_regex = filter_regex + self.previous_measurements = self.load_previous_measurements_from_json(compilation_path) + + @staticmethod + def load_previous_measurements_from_json(compilation_path: Traversable) -> list[str]: + previous_measurements = [] + for reference_dir in compilation_path.iterdir(): + if not reference_dir.is_dir(): + continue + for json_file in reference_dir.iterdir(): + if '.json' not in str(json_file): + continue + with open(json_file, "r", encoding="utf-8") as f: + previous_measurements.extend(json.load(f).keys()) + + return sorted(previous_measurements) + + # CHATGPT generated. TODO: Double check this works as intended. + def create_widget(self, frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + # --- filter entry --- + filter_var = tk.StringVar() + filter_var.set(self.filter_regex) + filter_entry = ttk.Entry(container, width=40, textvariable=filter_var) + filter_entry.grid(row=0, column=0, columnspan=2, sticky="w") + + # --- scrollable checklist --- + canvas = tk.Canvas(container, height=150) + scrollbar = ttk.Scrollbar(container, orient="vertical", command=canvas.yview) + checklist_frame = ttk.Frame(canvas) + + canvas.configure(yscrollcommand=scrollbar.set) + + canvas.grid(row=1, column=0, sticky="nsew") + scrollbar.grid(row=1, column=1, sticky="ns") + + canvas.create_window((0, 0), window=checklist_frame, anchor="nw") + + # --- checkbox state --- + vars_by_key: dict[str, tk.BooleanVar] = {} + checkbox_widgets: dict[str, ttk.Checkbutton] = {} + + for data_key in self.previous_measurements: + var = tk.BooleanVar(value=False) + check = ttk.Checkbutton( + checklist_frame, + text=data_key, + variable=var + ) + check.pack(anchor="w") + vars_by_key[data_key] = var + checkbox_widgets[data_key] = check + + def update_scrollregion(*_): + canvas.configure(scrollregion=canvas.bbox("all")) + + checklist_frame.bind("", update_scrollregion) + + # --- regex filtering logic --- + def filter_list(*_): + pattern = filter_var.get() + try: + regex = re.compile(pattern, re.IGNORECASE) + except re.error: + # Invalid regex: hide everything + for chk in checkbox_widgets.values(): + chk.pack_forget() + update_scrollregion() + return + + for key, chk in checkbox_widgets.items(): + if regex.search(key): + chk.pack(anchor="w") + else: + chk.pack_forget() + + filter_list() + update_scrollregion() + + filter_var.trace_add("write", filter_list) + + # --- select / deselect buttons --- + button_frame = ttk.Frame(container) + button_frame.grid(row=2, column=0, columnspan=2, sticky="w", pady=(4, 0)) + + def select_visible(state: bool): + for key, chk in checkbox_widgets.items(): + if chk.winfo_manager(): # only visible (i.e., packed) widgets + vars_by_key[key].set(state) + + ttk.Button( + button_frame, + text="Select all", + command=lambda: select_visible(True), + width=12, + ).pack(side="left", padx=(0, 4)) + + ttk.Button( + button_frame, + text="Deselect all", + command=lambda: select_visible(False), + width=12, + ).pack(side="left") + + container.selection_vars = vars_by_key + return container + + +class ReferenceWidgetcreator: + _reference_options: list[str] + + def __init__(self, references: dict | None = None, reference_path: Traversable | None = None): + if references is None and reference_path is None: + return + if references is not None and reference_path is not None: + raise ValueError('Both references and reference_file supplied to ReferenceWidgetcreator.') + elif references is not None: + self.references = references + self.reference_path = None + else: + self.load_references_from_json(reference_path) + + # ---------- file helpers ---------- + def load_references_from_json(self, reference_path: Traversable): + self.reference_path = reference_path + with open(reference_path, "r", encoding="utf-8") as f: + self.references = json.load(f) + + def _save_references(self, data: dict): + with open(self.reference_path, "w", encoding="utf-8") as f: + json.dump(data, f, indent=4) + + @property + def reference_options(self): + return self._reference_options + + @reference_options.getter + def reference_options(self): + return sorted(self.references) + + # Main widget! + def create_widget(self, frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + combo = ttk.Combobox( + container, + width=40, + state="normal", + values=self.reference_options + ) + combo.grid(row=0, column=0, pady=4) + + def filter_references(_): + typed = combo.get().lower() + filtered = [ + key for key in self.reference_options + if typed in key.lower() + ] + combo["values"] = filtered + + combo.bind("", filter_references) + + def auto_complete(_): + typed = combo.get().lower() + filtered = [name for name in self.reference_options if typed in name.lower()] + if filtered: + combo.set(filtered[0]) + + combo.bind("", auto_complete) + + add_new = ttk.Button( + container, + text="New Ref", + command=lambda: self._open_new_reference_form(combo) + ) + add_new.grid(row=0, column=1, padx=(6, 0)) + + return combo + + def _open_new_reference_form(self, combo: ttk.Combobox): + win = tk.Toplevel() + win.title("Add New Reference") + win.transient() + win.grab_set() + + fields = [ + ("Title", "title"), + ("Authors (one per line)", "author"), + ("Year", "year"), + ("Month", "month"), + ("Journal", "journal"), + ("Volume", "volume"), + ("Pages", "pages"), + ("URL", "url"), + ("DOI", "doi"), + ] + + entries = OrderedDict() + + long_entries = {'Title', 'Authors (one per line)'} + + for row, (label, key) in enumerate(fields): + ttk.Label(win, text=label).grid(row=row, column=0, sticky="w", pady=4, padx=4) + if label not in long_entries: + entry = tk.Entry(win, width=50) + else: + entry = scrolledtext.ScrolledText(win, width=50, height=3) + + def focus_next_widget(event): + event.widget.tk_focusNext().focus() + return "break" + + entry.bind("", focus_next_widget) + + entry.grid(row=row, column=1, pady=4, padx=4) + entries[key] = entry + + # ---------- submit logic ---------- + def submit(): + try: + authors = [ + a.strip() + for a in entries["author"].get("1.0", 'end-1c').splitlines() + if a.strip() + ] + if not authors: + raise ValueError("At least one author is required") + + year = entries["year"].get().strip() + if not year: + raise ValueError("Year is required") + + title = entries['title'].get("1.0", 'end-1c') + citation_key = authors[0].split()[-1].lower() + '_' + title.lower().split()[0] + '_' + year + + references = self.references + if citation_key in references: + raise ValueError(f"Reference '{citation_key}' already exists") + + references[citation_key] = { + "title": title, + "author": authors, + "year": year, + "month": entries["month"].get() or None, + "journal": entries["journal"].get() or None, + "volume": entries["volume"].get(), + "pages": entries["pages"].get(), + "url": entries["url"].get() or None, + "doi": entries["doi"].get() or None, + } + + self._save_references(references) + + # update combobox + combo["values"] = self.reference_options + combo.set(citation_key) + + win.destroy() + + except ValueError as e: + messagebox.showerror("Invalid Reference", str(e), parent=win) + + ttk.Button(win, text="Submit", command=submit).grid( + row=len(fields), column=0, columnspan=2, pady=10 + ) + + @staticmethod + def _parse_int(value: str): + value = value.strip() + return int(value) if value else None + + +class SelectWidgetCreator: + def __init__(self, options: list[str]): + if not options: + raise ValueError("SelectWidgetCreator requires a non-empty options list") + self.options = options + + def create_widget(self, frame, row) -> tk.Widget: + combo = ttk.Combobox( + frame, + values=self.options, + state="readonly", + width=40 + ) + combo.grid(row=row, column=1, pady=4, sticky="w") + + # auto-select first option + combo.current(0) + + return combo + + +class TransitionWidgetCreator: + + @staticmethod + def create_widget(frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, pady=4, sticky="w") + + upper_entry = ttk.Entry(container, width=18) + lower_entry = ttk.Entry(container, width=18) + + upper_entry.grid(row=0, column=0, padx=(0, 5)) + ttk.Label(container, text="→").grid(row=0, column=1) + lower_entry.grid(row=0, column=2, padx=(5, 0)) + + # Attach for processor access + container.upper_entry = upper_entry + container.lower_entry = lower_entry + + return container + + +class MultiTransitionWidgetCreator: + + @staticmethod + def create_widget(frame, row): + + class MultiContainer(ttk.Frame): # Mainly for type hinting + def __init__(self, transition_entries, buttons, *args, **kwargs): + super().__init__(frame, *args, **kwargs) + self.transition_entries: list[tuple[tk.Label, tk.Frame]] = transition_entries + self.buttons: list[tk.Button] = buttons + + def regrid(self): + for i, (label, transition_frame) in enumerate(self.transition_entries): + label.grid(row=i), transition_frame.grid(row=i) + for button in self.buttons: + button.grid(row=len(self.transition_entries)) + + container = MultiContainer(transition_entries=[], buttons=[]) + container.grid(row=row, column=1, pady=4, sticky="w") + + def add_new_transition(*_): + number_of_rows = len(container.transition_entries) + new_letter = f'{chr(ord("A") + number_of_rows)}' + + label = tk.Label(container, text=f'{new_letter}') + label.grid(row=number_of_rows, column=0) + + transition_frame = ttk.Frame(container) # Contains label and transition_frame + transition_frame.grid(row=number_of_rows, column=1) + + upper_entry = ttk.Entry(transition_frame, width=18) + lower_entry = ttk.Entry(transition_frame, width=18) + + upper_entry.grid(row=0, column=0, padx=(0, 5)) + ttk.Label(transition_frame, text="→").grid(row=0, column=1) + lower_entry.grid(row=0, column=2, padx=(5, 0)) + + transition_frame.upper_entry = upper_entry + transition_frame.lower_entry = lower_entry + + container.transition_entries.append((label, transition_frame)) + container.regrid() + + def delete_transition(*_): + label, transition_frame = container.transition_entries.pop() + label.grid_forget(), transition_frame.grid_forget() + container.regrid() + + add_button = ttk.Button(container, text="Add", command=add_new_transition, takefocus=0) + add_button.grid(row=0, column=0, pady=10) + + delete_button = ttk.Button(container, text="Remove", command=delete_transition, takefocus=0) + delete_button.grid(row=0, column=1, pady=10) + container.buttons = [add_button, delete_button] + add_new_transition(), add_new_transition() + + return container + + +class FieldSpec(NamedTuple): + name: str + processor: FieldProcessor + widget_creator: Widgetcreator = DefaultWidgetcreator() + hovertext: str | None = None + + +class InputTemplate(NamedTuple): + name: str + fields: list[FieldSpec] + data_key: Callable[[dict[str, Any]], str] + + +# Useful fields that get reused +reference_field = FieldSpec("Reference", ReferenceProcessor(reference_path=config['reference_path']), + ReferenceWidgetcreator(reference_path=config['reference_path'])) + +nuclide_field = FieldSpec("Nuclide", NuclideProcessor(), hovertext='Provide a nuclide in the format Pb208') + +transition_field = FieldSpec("Transition", TransitionProcessor(), TransitionWidgetCreator(), + hovertext='Enter the upper and lower levels of the atomic/muonic transition') + +notes_field = FieldSpec("Notes", CastProcessor(str, allows_empty=True)) + +# LIST TEMPLATES HERE. Each template must include a FieldSpec named "Reference". +muonic_transition_energy_template = InputTemplate( + name="Muonic Transition Energy", + fields=[ + reference_field, + nuclide_field, + transition_field, + FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'muonic', values['Nuclide'], + values['Transition']['Upper'], values['Transition']['Lower']])) + +muonic_transition_energy_difference_template = InputTemplate( + name="Muonic Transition Energy Difference (different nuclides)", + fields=[ + reference_field, + FieldSpec("Nuclide A", NuclideProcessor()), + FieldSpec("Nuclide B", NuclideProcessor()), + transition_field, + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'muonic_difference', values['NuclideA'], values['NuclideB'], + values['Transition']['Upper'], values['Transition']['Lower']]) +) + +muonic_transition_energy_difference_diff_transition_template = InputTemplate( + name="Muonic Transition Energy Difference (different transitions)", + fields=[ + reference_field, + nuclide_field, + FieldSpec("Transitions", MultiTransitionProcessor(), MultiTransitionWidgetCreator(), + hovertext='Enter the upper and lower levels of the atomic/muonic transition'), + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'muonic_difference', values['Nuclide'], + *list(sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values['Transitions'].items()], ()))]) +) + +muonic_barret_theory_template = InputTemplate( + name="Muonic Barrett Moment", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + FieldSpec('Rka [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('k [-]', CastProcessor(str)), + FieldSpec('alpha [1/fm]', CastProcessor(str)), + FieldSpec('Cz [fm/keV]', CastProcessor(str)), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'barrett_moment', values['Nuclide'], + *['-'.join(s.split('_')[-2:]) for s in + values['Previous Muonic Measurements']]]) +) + +muonic_radius_template = InputTemplate( + name="Muonic Radius", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + FieldSpec('R [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('Nuclear Polarization Method', SelectProcessor(['Calculated', 'Fit']), + SelectWidgetCreator(['Calculated', 'Fit']), + hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), + FieldSpec('Reduced Chi-Squared', CastProcessor(float, allows_empty=True)), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'radius', values['Nuclide'], + 'NP', values['Nuclear Polarization Method']]) +) + +muonic_fermi_distribution_template = InputTemplate( + name="Fermi Distribution", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousMeasurementProcessor(), + PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + nuclide_field, + # TODO add fermi distribution processor and widget creator with different fermi distribution options. + FieldSpec('c [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('a [fm]', NumberWithUncertaintyProcessor()), + notes_field + ], + data_key=lambda values: '_'.join([values['Reference'], 'fermi', values['Nuclide']]) +) + +templates = [muonic_transition_energy_template, + muonic_transition_energy_difference_template, + muonic_transition_energy_difference_diff_transition_template, + muonic_barret_theory_template, + muonic_radius_template, + muonic_fermi_distribution_template] + + +class DataEntryInterface: + templates: list[InputTemplate] + current_entries: OrderedDict[str, tuple[tk.Widget, FieldProcessor]] + references: dict[str, Reference] + reference_path: Traversable | None + compilation_folder: Traversable + + def __init__(self, + references: dict[str, Reference] | Traversable | None = None, + compilation_folder: Optional[str | Traversable] = None): + + self.root = tk.Tk() + self.root.title("Data Entry Interface") + + def _on_mousewheel(event): + widget = event.widget + try: + widget.yview_scroll(int(-1 * (event.delta / 120)), "units") + except AttributeError: + pass + + self.root.bind_all("", _on_mousewheel) + + if references is None: + self._load_references_from_json(config['reference_path']) + elif isinstance(references, Traversable): + self._load_references_from_json(references) + elif isinstance(references, dict): + self.reference_path = None + self.references = references + + compilation_folder = compilation_folder if compilation_folder is not None else config['compilation_dir'] + self.compilation_folder = Path(compilation_folder) if not isinstance(compilation_folder, + Traversable) else compilation_folder + + # Register templates here + self.templates = templates + + self.last_submitted = tk.StringVar() + self.field_widgets = {} # field_name -> widget + self.keep_vars = {} # field_name -> BooleanVar + + self.current_entries: OrderedDict[ + str, tuple[tk.Widget, FieldProcessor]] = OrderedDict() # Stores tk entry objects for each field displayed. + self.show_template_selection() + + def _load_references_from_json(self, reference_path: Optional[str | Traversable] = None): + with open(reference_path, "r", encoding="utf-8") as f: + raw_refs = json.load(f) + + self.reference_path = reference_path + self.references = {key: Reference(**value) for key, value in raw_refs.items()} + + def clear_window(self): + for widget in self.root.winfo_children(): + widget.destroy() + + def show_template_selection(self): + self.clear_window() + + ttk.Label( + self.root, + text="Select Data Entry Template", + font=("Arial", 16, "bold") + ).pack(pady=10) + + self.template_var = tk.StringVar() + + names = [t.name for t in self.templates] + + template_combo = ttk.Combobox( + self.root, + textvariable=self.template_var, + values=names, + font=("Arial", 12), + state="readonly", + width=60 + ) + template_combo.pack(pady=5) + + ttk.Button( + self.root, + text="Continue", + command=self.load_selected_template + ).pack(pady=10) + + def load_selected_template(self): + selected_name = self.template_var.get() + if not selected_name: + messagebox.showerror("Error", "Please select a template.") + return + + for template in self.templates: + if template.name == selected_name: + self.display_input(template) + return + + def display_input(self, template: InputTemplate): + self.clear_window() + self.current_entries.clear() + + ttk.Label( + self.root, + text=template.name, + font=("Arial", 16, "bold"), + wraplength=300 + ).pack(pady=10) + + form_frame = ttk.Frame(self.root) + form_frame.pack(padx=10, pady=10, fill="x") + + for row, field in enumerate(template.fields): + label = ttk.Label(form_frame, + text=field.name, + font=("Arial", 11), + wraplength=120 + ) + label.grid(row=row, column=0, sticky='w', pady=4) + if field.hovertext: + ToolTip(label, field.hovertext) + + entry = field.widget_creator.create_widget(form_frame, row) + self.current_entries[field.name] = (entry, field.processor) + + keep_var = tk.BooleanVar(value=False) + self.keep_vars[field.name] = keep_var + + keep_check = ttk.Checkbutton( + form_frame, + text="Keep", + variable=keep_var, + takefocus=0 + ) + keep_check.grid(row=row, column=2, padx=(6, 0)) + + button_frame = ttk.Frame(self.root) + button_frame.pack(pady=10) + + submit = ttk.Button( + button_frame, + text="Submit", + command=lambda: self.submit_data(template) + ) + submit.grid(row=0, column=0, padx=5) + submit.bind("", lambda _: self.submit_data(template)) + + ttk.Button( + button_frame, + text="Back", + command=self.show_template_selection + ).grid(row=0, column=1, padx=5) + + ttk.Button( + button_frame, + text="2D", + command=lambda: self.select_for_twod_input(template) + ).grid(row=0, column=2, padx=5) + + ttk.Label( + button_frame, + textvariable=self.last_submitted, + font=("Arial", 10) + ).grid(row=1, column=0, pady=3) + + def select_for_twod_input(self, template): + dialog = tk.Toplevel(self.root) + dialog.title("2D Input Selection") + dialog.transient(self.root) + dialog.grab_set() + + ttk.Label( + dialog, + text="Select the fields you would like to form the row index, column index, and the value you want to enter " + "for each row/column pair.", + wraplength=400, + justify="left" + ).pack(padx=20, pady=15) + + field_names = [field.name for field in template.fields] + btn_frame = ttk.Frame(dialog) + btn_frame.pack(fill="both", expand=True, padx=20, pady=10) + buttons = [] + + for i, selection in enumerate(['Row Field', 'Column Field', 'Value Field']): + tk.Label(btn_frame, text=selection).grid(row=i, column=0) + button = SelectWidgetCreator(field_names).create_widget(btn_frame, row=i) + buttons.append(button) + + def create_2d(): + field_answers = [btn.get() for btn in buttons] + dialog.destroy() + self.twod_input(template, *field_answers) + + ttk.Button(btn_frame, text="Create 2D", + command=create_2d).grid(row=3, column=0, padx=5) + ttk.Button(btn_frame, text="Back", command=lambda: dialog.destroy()).grid(row=3, column=1, padx=5) + + self.root.wait_window(dialog) + + def twod_input(self, template, row_field, col_field, value_field): + dialog = tk.Toplevel(self.root) + dialog.title(f"2D Input Selection: Values={value_field}") + dialog.transient(self.root) + dialog.grab_set() + + frame = ttk.Frame(dialog) + frame.pack(fill="both", expand=True, padx=10, pady=10) + + ttk.Label(frame, text=row_field).grid(row=1, column=0, padx=5, pady=5) + ttk.Label(frame, text=col_field).grid(row=0, column=1, padx=5, pady=5) + + grid_frame = ttk.Frame(frame) + grid_frame.grid(row=1, column=1) + + row_btn_frame = ttk.Frame(frame) + row_btn_frame.grid(row=2, column=0, sticky="n") + ttk.Button(row_btn_frame, text="+", command=lambda: grow_grid(rows=1, columns=0)).pack() + ttk.Button(row_btn_frame, text="-", command=lambda: shrink_grid(rows=1, columns=0)).pack() + + col_btn_frame = ttk.Frame(frame) + col_btn_frame.grid(row=0, column=2, sticky="e") + ttk.Button(col_btn_frame, text="+", command=lambda: grow_grid(rows=0, columns=1)).pack(side="left") + ttk.Button(col_btn_frame, text="-", command=lambda: shrink_grid(rows=0, columns=1)).pack(side="left") + + main_btn_frame = ttk.Frame(frame) + main_btn_frame.grid(row=0, column=0, sticky='w') + tk.Button(main_btn_frame, text='Submit', + command=lambda: self.submit_2d(template, row_field, col_field, value_field, row_widgets, col_widgets, cells)).pack() + tk.Button(main_btn_frame, text='Back', command=lambda: dialog.destroy()).pack() + + row_widgets: list[tk.Widget] = [] + col_widgets: list[tk.Widget] = [] + cells: list[list[tk.Widget]] = [] + + def make_widget(field_name): + field, = [field for field in template.fields if field.name == field_name] + return field.widget_creator.create_widget(grid_frame, row=0) + + def regrid(): + for w in grid_frame.winfo_children(): + w.grid_forget() + + # Column headers + for j, cw in enumerate(col_widgets): + cw.grid(row=0, column=j + 1, padx=5, pady=5, sticky="nsew") + grid_frame.columnconfigure(j + 1, weight=1) + + # Row headers + cells + for i, rw in enumerate(row_widgets): + rw.grid(row=i + 1, column=0, padx=5, pady=5, sticky="nsew") + grid_frame.rowconfigure(i + 1, weight=1) + + for j, cell in enumerate(cells[i]): + cell.grid(row=i + 1, column=j + 1, padx=5, pady=5, sticky="nsew") + cell.bind("", lambda e, fi=i, fj=j: (cells[fi][(fj + 1) % len(cells[fi])].focus(), "break")[1]) + cell.bind("", lambda e, fi=i, fj=j: (cells[(fi + 1) % len(cells)][fj].focus(), "break")[1]) + + def grow_grid(rows, columns): + if rows: + rw = make_widget(row_field) + rw.config(takefocus=0) + row_widgets.append(rw) + + new_row = [make_widget(value_field) for _ in col_widgets] + cells.append(new_row) + + if columns: + cw = make_widget(col_field) + cw.config(takefocus=0) + col_widgets.append(cw) + + for row in cells: + row.append(make_widget(value_field)) + + regrid() + + def shrink_grid(rows, columns): + if rows and row_widgets: + row_widgets.pop().destroy() + for cell in cells.pop(): + cell.destroy() + + if columns and col_widgets: + col_widgets.pop().destroy() + for row in cells: + row.pop().destroy() + + regrid() + + grow_grid(rows=2, columns=2) + + def submit_2d(self, template, row_field, col_field, value_field, row_widgets, col_widgets, cells): + # We take each (row_widget, col_widget, cell_widget) triplet, fill them in to the main data entry tab, + # and trigger the data submission. + + original_entries = {field_name: self.current_entries[field_name] for field_name in (row_field, col_field, value_field)} + + for row_widget, cell_row in zip(row_widgets, cells): + for col_widget, cell in zip(col_widgets, cell_row): + for field_name, widget in [(row_field, row_widget), (col_field, col_widget), (value_field, cell)]: + prev_entry, processor = self.current_entries[field_name] + self.current_entries[field_name] = (widget, processor) + self.submit_data(template, clear_fields=False) # We don't want to erase our row/col entries as we submit + + for field_name in (row_field, col_field, value_field): # make sure we restore the original widgets once we are done submitting. + self.current_entries[field_name] = original_entries[field_name] + + pass + + def submit_data(self, template: InputTemplate, clear_fields=True): + + def clear_widget(widg: tk.Widget): + if isinstance(widg, ttk.Entry): + widg.delete(0, tk.END) + return + + # Composite widgets (e.g. Transition frame) + for child in widget.winfo_children(): + if isinstance(child, ttk.Entry): + child.delete(0, tk.END) + + data = OrderedDict() + + try: + for field_name, (widget, processor) in self.current_entries.items(): + data[field_name] = processor.process(widget) + except ValueError as e: + messagebox.showerror("Invalid Input", str(e)) + return + + self.save_data(template, data) + + focus_widget = None + for field_name, (widget, _) in self.current_entries.items(): + if not self.keep_vars[field_name].get() and clear_fields: + clear_widget(widget) + if focus_widget is None: + widget.focus() + focus_widget = widget + + self.last_submitted.set(f'Last Submitted: {template.data_key(data)}') + + def save_data( + self, + template: InputTemplate, + data: dict, + replacement_strategy: Literal["Ask", "AlwaysReplace", "NeverReplace"] = "Ask", + ) -> None: + + data_key = template.data_key(data) + file_dir = self.compilation_folder / data["Reference"] + file_dir.mkdir(parents=True, exist_ok=True) + + file = file_dir / f"{template.name}.json" + + new_entry = {data_key: data} + + if file.exists(): + with file.open("r", encoding="utf-8") as f: + existing_data = json.load(f) + + if data_key in existing_data: + match replacement_strategy: + case "AlwaysReplace": + existing_data[data_key] = data + + case "NeverReplace": + return + + case "Ask": + action = self._ask_collision_action(self.root, data_key, file) + + if action == "replace": + existing_data[data_key] = data + + elif action == "suffix": + new_key = self._next_available_key(data_key, existing_data) + existing_data[new_key] = data + + else: # do nothing + return + else: + existing_data[data_key] = data + + data_to_write = existing_data + + else: + data_to_write = new_entry + + with file.open("w", encoding="utf-8") as f: + json.dump(data_to_write, f, indent=4) + + print(f"Data successfully saved to {file}") + + @staticmethod + def _next_available_key(base_key: str, existing: dict) -> str: + suffix = ord("a") + while True: + candidate = f"{base_key}_{chr(suffix)}" + if candidate not in existing: + return candidate + suffix += 1 + + @staticmethod + def _ask_collision_action(parent, key: str, file: Path) -> str | None: + """ + Returns: 'replace', 'suffix', or None (do nothing) + """ + result = None + dialog = tk.Toplevel(parent) + dialog.title("Duplicate Entry") + dialog.transient(parent) + dialog.grab_set() + + ttk.Label( + dialog, + text=f"'{key}' already exists in:\n{file}\n\nWhat would you like to do?", + wraplength=400, + justify="left" + ).pack(padx=20, pady=15) + + def choose(action): + nonlocal result + result = action + dialog.destroy() + + btns = ttk.Frame(dialog) + btns.pack(pady=10) + + ttk.Button(btns, text="Replace", command=lambda: choose("replace")).grid(row=0, column=0, padx=5) + ttk.Button(btns, text="Add Suffix", command=lambda: choose("suffix")).grid(row=0, column=1, padx=5) + ttk.Button(btns, text="Do Nothing", command=lambda: choose(None)).grid(row=0, column=2, padx=5) + + parent.wait_window(dialog) + return result + + +if __name__ == "__main__": + interface = DataEntryInterface(references=config['reference_path']) + interface.root.mainloop() diff --git a/radbase/radius_analyzer.py b/radbase/radius_analyzer.py index 46273b6..4439492 100644 --- a/radbase/radius_analyzer.py +++ b/radbase/radius_analyzer.py @@ -13,40 +13,7 @@ from lmfit import Minimizer, Parameters from uncertainties import correlated_values_norm, correlation_matrix, ufloat -from .converter import Measurement - - -class Nuclide: - z: int - a: int - - def __init__(self, nucstr): - self.nucstr = nucstr - nucstr = nucstr[1:] - self.z = int(nucstr[:3]) - self.a = int(nucstr[3:]) - self.n = self.a - self.z - - def guess_radius(self): - # semiempirical estimate - return (0.9071 + 1.1025 / (self.a ** (2 / 3)) + -0.548 / (self.a ** (4 / 3))) * self.a ** (1 / 3) - - def __repr__(self): - return f'Nuclide (Z={self.z}, A={self.a})' - - def __eq__(self, other): - return (self.z == other.z) and (self.a == other.a) - - def __lt__(self, other): - if self.z != other.z: - return self.z < other.z - return self.a < other.a - - def __hash__(self): - return self.z * 1000 + self.a - - def __str__(self): - return f'R{self.z:03}{self.a:03}' +from .converter import Measurement, Nuclide class Term: diff --git a/tests/test_converter.py b/tests/test_converter.py new file mode 100644 index 0000000..b3f6d02 --- /dev/null +++ b/tests/test_converter.py @@ -0,0 +1,4 @@ + +from uncertainties import ufloat + +from radbase.converter import Quantity, QuantityType diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py new file mode 100644 index 0000000..2eea918 --- /dev/null +++ b/tests/test_data_entry.py @@ -0,0 +1,156 @@ +import json +# Allows for +import os +import pathlib +import tkinter as tk +from tkinter import ttk + +import pytest + +from radbase.data_entry import (CastProcessor, DataEntryInterface, FieldSpec, + InputTemplate, NuclideProcessor, + NumberWithUncertaintyProcessor, + ReferenceProcessor, templates) + +if os.environ.get('DISPLAY','') == '': + print('no display found. Using :0.0') + os.environ.__setitem__('DISPLAY', ':0.0') + +example_references = { + "Smith_nuclear_1978": { + "title": "Nuclear Charge Radii from Muonic Atoms", + "author": ["John Smith", "Alice Jones"], + "year": "1978", + }, + "Brown_isotope_1992": { + "title": "Isotope Shifts in Heavy Nuclei", + "author": ["Michael Brown"], + "year": "1992" + } +} + +# Maps field names in data_entry.templates to example outputs. +example_outputs = { + 'Reference': list(example_references.keys())[0], + 'Previous Muonic Measurements': list(example_references.keys())[0] + '_muonic_2p1/2_1s1/2', + 'Nuclide': 'Pb208' + '' + + +} + + +def make_dummy_references(tmp_path): + temp_references_file = tmp_path / 'references.json' + temp_references_file.write_text(json.dumps(example_references)) + return temp_references_file + + +class DummyProcessor: + @staticmethod + def process(widget): + return 'nothing' + + +dummy_template = InputTemplate(name='test', + fields=[FieldSpec('Reference', CastProcessor(str)), + FieldSpec('testfield', DummyProcessor())], + data_key=lambda x: 'testkey') + + +class DummyWidget(ttk.Widget): + def __init__(self, value): + self.value = value + + def get(self): + return self.value + + +def test_cast_processor(): + widget = DummyWidget('30.2') + blank_widget = DummyWidget('') + + assert CastProcessor(str).process(widget) == '30.2' + assert CastProcessor(float).process(widget) == 30.2 + + with pytest.raises(ValueError) as e_info: # should raise error if it can not cast + CastProcessor(int).process(widget) + with pytest.raises(ValueError) as e_info: # should raise error if field was left blank. + CastProcessor(str).process(blank_widget) + + +def test_nuclide_processor(): + widget = DummyWidget('Pb208') + natwidget = DummyWidget('Pbnat') + bad_widget = DummyWidget('082203') + + assert NuclideProcessor().process(widget) == 'Pb208' + assert NuclideProcessor().process(natwidget) == 'Pbnat' + with pytest.raises(ValueError) as e_info: + NuclideProcessor().process(bad_widget) + + +def test_reference_processor(tmp_path): + + global example_references + + good_widget = DummyWidget('Smith_nuclear_1978') + bad_widget = DummyWidget('Noone_title_1340') + + tmp_ref_path = make_dummy_references(tmp_path) + ref_proc = ReferenceProcessor(tmp_ref_path) + + assert ref_proc.process(good_widget) == 'Smith_nuclear_1978' + with pytest.raises(ValueError) as e_info: + ref_proc.process(bad_widget) + + +def test_number_with_uncertainty_processor(): + + float_widget = DummyWidget('100.1') + uncertainty_widget = DummyWidget('100.1(3)') + bad_widget = DummyWidget('bad') + + ref_proc = NumberWithUncertaintyProcessor() + + assert ref_proc.process(float_widget) == {'value': 100.1, 'uncertainty': None} + assert ref_proc.process(uncertainty_widget) == {'value': 100.1, 'uncertainty': 0.3} + with pytest.raises(ValueError) as e_info: + ref_proc.process(bad_widget) + + +def test_init_data_entry_interface(tmp_path): + + global example_references + + temp_references_file = tmp_path / 'references.json' + temp_references_file.write_text(json.dumps(example_references)) + + DataEntryInterface() + + +def test_save_data(tmp_path): + + ref_key = list(example_references.keys())[0] + test_data = {'Reference': ref_key, 'testfield': 3} + tmp_path.mkdir(exist_ok=True) + tmp_data_loc = tmp_path / ref_key / f'{dummy_template.name}.json' + + interface = DataEntryInterface(compilation_folder=tmp_path) + + interface.save_data(dummy_template, test_data, replacement_strategy='AlwaysReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': test_data} + + new_test_data = test_data.copy() + new_test_data['testfield'] = 5 + interface.save_data(dummy_template, new_test_data, replacement_strategy='AlwaysReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': new_test_data} + + interface.save_data(dummy_template, test_data, replacement_strategy='NeverReplace') + assert json.loads(tmp_data_loc.read_text()) == {'testkey': new_test_data} + + +# def test_previous_measurement_processor(tmp_path): +# +# previous_measurements = {'Authors'} +# proc = PreviousMeasurementProcessor(previous_measurements = {}) From 5bae2e35fafd8f281fb755f6f1954afb97b07859 Mon Sep 17 00:00:00 2001 From: Hunter Date: Wed, 11 Feb 2026 11:50:34 -0500 Subject: [PATCH 04/11] Added flexible fields (VariableNumberProcessor), entered data --- .../Fermi Distribution.json | 50 + ...alculated Muonic Nuclear Polarization.json | 32 + .../piller_nuclear_1990/Muonic Radius.json | 22 + .../Muonic Transition Energy.json | 28 + ...nergy Difference (different nuclides).json | 58 + .../Muonic Transition Energy.json | 67 + radbase/compilation/references.json | 89 + ...alculated Muonic Nuclear Polarization.json | 210 ++ ...nergy Difference (different nuclides).json | 1682 +++++++++++++++++ .../Muonic Transition Energy.json | 301 +++ ...alculated Muonic Nuclear Polarization.json | 22 + .../test_test_1700/Muonic Radius.json | 43 + ...nergy Difference (different nuclides).json | 30 + .../Muonic Transition Energy.json | 107 +- radbase/data_entry.py | 472 ++++- radbase/startup/compare_to_angeli.py | 4 +- readme.rst | 13 +- tests/test_data_entry.py | 120 +- 18 files changed, 3136 insertions(+), 214 deletions(-) create mode 100644 radbase/compilation/johnson_241am_1985/Fermi Distribution.json create mode 100644 radbase/compilation/piller_nuclear_1990/Calculated Muonic Nuclear Polarization.json create mode 100644 radbase/compilation/piller_nuclear_1990/Muonic Radius.json create mode 100644 radbase/compilation/piller_nuclear_1990/Muonic Transition Energy.json create mode 100644 radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy Difference (different nuclides).json create mode 100644 radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy.json create mode 100644 radbase/compilation/shera_systematics_1976/Calculated Muonic Nuclear Polarization.json create mode 100644 radbase/compilation/shera_systematics_1976/Muonic Transition Energy Difference (different nuclides).json create mode 100644 radbase/compilation/shera_systematics_1976/Muonic Transition Energy.json create mode 100644 radbase/compilation/test_test_1700/Calculated Muonic Nuclear Polarization.json create mode 100644 radbase/compilation/test_test_1700/Muonic Radius.json create mode 100644 radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different nuclides).json diff --git a/radbase/compilation/johnson_241am_1985/Fermi Distribution.json b/radbase/compilation/johnson_241am_1985/Fermi Distribution.json new file mode 100644 index 0000000..56cebee --- /dev/null +++ b/radbase/compilation/johnson_241am_1985/Fermi Distribution.json @@ -0,0 +1,50 @@ +{ + "johnson_241am_1985_fermi_Am241": { + "Reference": "johnson_241am_1985", + "Relies On": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" + ], + "Nuclide": "Am241", + "c [fm]": { + "value": 7.1865, + "uncertainty": 0.0004 + }, + "a [fm]": { + "value": 0.522, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.298, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.057, + "uncertainty": null + }, + "Notes": "Beta2, Beta4 from OIS; Experimental uncertainties only" + }, + "johnson_241am_1985_fermi_Am243": { + "Reference": "johnson_241am_1985", + "Relies On": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" + ], + "Nuclide": "Am243", + "c [fm]": { + "value": 7.2048, + "uncertainty": 0.0004 + }, + "a [fm]": { + "value": 0.522, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.296, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.037, + "uncertainty": null + }, + "Notes": "Beta2, Beta4 from OIS; Experimental uncertainties only" + } +} diff --git a/radbase/compilation/piller_nuclear_1990/Calculated Muonic Nuclear Polarization.json b/radbase/compilation/piller_nuclear_1990/Calculated Muonic Nuclear Polarization.json new file mode 100644 index 0000000..1d4bbd8 --- /dev/null +++ b/radbase/compilation/piller_nuclear_1990/Calculated Muonic Nuclear Polarization.json @@ -0,0 +1,32 @@ +{ + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2": { + "Reference": "piller_nuclear_1990", + "Nuclide": "Sn112", + "Level": "1s1/2", + "Energy [keV]": { + "value": 1.755, + "uncertainty": null + }, + "Notes": "" + }, + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2": { + "Reference": "piller_nuclear_1990", + "Nuclide": "Sn112", + "Level": "2p1/2", + "Energy [keV]": { + "value": 0.255, + "uncertainty": null + }, + "Notes": "" + }, + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2": { + "Reference": "piller_nuclear_1990", + "Nuclide": "Sn112", + "Level": "2p3/2", + "Energy [keV]": { + "value": 0.226, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/piller_nuclear_1990/Muonic Radius.json b/radbase/compilation/piller_nuclear_1990/Muonic Radius.json new file mode 100644 index 0000000..804a1a6 --- /dev/null +++ b/radbase/compilation/piller_nuclear_1990/Muonic Radius.json @@ -0,0 +1,22 @@ +{ + "piller_nuclear_1990_radius_Sn112_NP_Calculated": { + "Reference": "piller_nuclear_1990", + "Relies On": [ + "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2", + "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2" + ], + "Nuclide": "Sn112", + "R [fm]": { + "value": 4.5958, + "uncertainty": 0.0005 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [ + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2" + ], + "Reduced Chi-Squared": 0.0, + "Notes": "Experimental uncertainty only" + } +} diff --git a/radbase/compilation/piller_nuclear_1990/Muonic Transition Energy.json b/radbase/compilation/piller_nuclear_1990/Muonic Transition Energy.json new file mode 100644 index 0000000..33f4704 --- /dev/null +++ b/radbase/compilation/piller_nuclear_1990/Muonic Transition Energy.json @@ -0,0 +1,28 @@ +{ + "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2": { + "Reference": "piller_nuclear_1990", + "Nuclide": "Sn112", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3432.564, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2": { + "Reference": "piller_nuclear_1990", + "Nuclide": "Sn112", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3478.531, + "uncertainty": 0.056 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy Difference (different nuclides).json new file mode 100644 index 0000000..9bdb57f --- /dev/null +++ b/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,58 @@ +{ + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p3/2_1s1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide_A": "Bi209", + "Nuclide_B": "Pb206", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 59.9, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p1/2_1s1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide_A": "Bi209", + "Nuclide_B": "Pb206", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 54.2, + "uncertainty": 2.0 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d5/2_2p3/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide_A": "Bi209", + "Nuclide_B": "Pb206", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 52.7, + "uncertainty": 2.0 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d3/2_2p1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide_A": "Bi209", + "Nuclide_B": "Pb206", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 57.3, + "uncertainty": 2.0 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy.json b/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy.json new file mode 100644 index 0000000..2747025 --- /dev/null +++ b/radbase/compilation/powers_hyperfine_1968/Muonic Transition Energy.json @@ -0,0 +1,67 @@ +{ + "powers_hyperfine_1968_muonic_Pb206_2p3/2_1s1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 5974.1, + "uncertainty": 2.0 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_Pb206_2p1/2_1s1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide": "Pb206", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 5789.0, + "uncertainty": 2.8 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_Pb206_3d5/2_2p3/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 2503.4, + "uncertainty": 2.3 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_Pb206_3d3/2_2p1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide": "Pb206", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2645.5, + "uncertainty": 2.3 + }, + "Notes": "" + }, + "powers_hyperfine_1968_muonic_Bi209_2p3/2_1s1/2": { + "Reference": "powers_hyperfine_1968", + "Nuclide": "Bi209", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 6034.0, + "uncertainty": 2.2 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json index a82f481..00faac5 100644 --- a/radbase/compilation/references.json +++ b/radbase/compilation/references.json @@ -66,5 +66,94 @@ "pages": "", "url": null, "doi": null + }, + "piller_nuclear_1990": { + "title": "Nuclear charge radii of the tin isotopes from muonic atoms", + "author": [ + "C. Piller", + "C. Gugler", + "R. Jacot-Guillarmod", + "L. A. Schaller", + "L. Schellenberg", + "H. Schneuwly", + "G. Fricke", + "T. Hennemann", + "J. Herberz" + ], + "year": "1990", + "month": "July", + "journal": "Physical Review C", + "volume": "42", + "pages": "182-189", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.42.182", + "doi": "10.1103/PhysRevC.42.182" + }, + "johnson_241am_1985": { + "title": "241Am AND 243Am CHARGE DISTRJBUTIONS FROM MUON IC X-RAY SPECTROSCOPY AND THE QUADRUPOLE MOMENT OF THE 240Am FISSION ISOMER", + "author": [ + "M.W. JOHNSON", + "E.B. SHERA", + "M.V. HOEHN", + "R.A. NAUMANN", + "J.D. ZUMBRO", + "C. E. BEMIS Jr." + ], + "year": "1985", + "month": "October", + "journal": "Physics Letters B", + "volume": "161", + "pages": "75-78", + "url": "https://www.sciencedirect.com/science/article/abs/pii/0370269385906124?via%3Dihub", + "doi": "10.1016/0370-2693(85)90612-4" + }, + "powers_muonlc_1974": { + "title": "MUONlC 197Au: A TEST OF THE WEAK-COUPLING MODEL", + "author": [ + "R. J . POWERS", + "P. MARTIN", + "G. H. MILLER", + "R. E. WELSH", + "D. A. JENKINS" + ], + "year": "1974", + "month": "February", + "journal": "Nuclear Physics A", + "volume": "230", + "pages": "413-445", + "url": "https://www.sciencedirect.com/science/article/abs/pii/037594747490147X", + "doi": "10.1016/0375-9474(74)90147-X\n" + }, + "powers_hyperfine_1968": { + "title": "Hyperfine ESects in Muonic Bi and Pb", + "author": [ + "R. J. Powers" + ], + "year": "1968", + "month": "May", + "journal": "The Physical Review", + "volume": "169", + "pages": "1-20", + "url": "https://journals.aps.org/pr/abstract/10.1103/PhysRev.169.1", + "doi": "10.1103/PhysRev.169.1" + }, + "shera_systematics_1976": { + "title": "Systematics of nuclear charge distributions in Fe, Co, Ni, Cu, and Zn deduced from muonic x-ray measurements", + "author": [ + "E. B. Shera", + "E. T. Ritter", + "R. B. Perkins", + "G. A. Rinker", + "L. K. Wagner", + "H. D. Wohlfahrt", + "G. Fricke", + "R. M. Steffen" + ], + "year": "1976", + "month": "August", + "journal": "Physical Review C", + "volume": "14", + "pages": "731-748", + "url": "10.1103/PhysRevC.14.731", + "doi": "https://link.aps.org/doi/10.1103/PhysRevC.14.731" } } diff --git a/radbase/compilation/shera_systematics_1976/Calculated Muonic Nuclear Polarization.json b/radbase/compilation/shera_systematics_1976/Calculated Muonic Nuclear Polarization.json new file mode 100644 index 0000000..f8c6ba0 --- /dev/null +++ b/radbase/compilation/shera_systematics_1976/Calculated Muonic Nuclear Polarization.json @@ -0,0 +1,210 @@ +{ + "shera_systematics_1976_muonic_nuclear_polarization_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.546, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.582, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.6, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.624, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.588, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.689, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.693, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.632, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.703, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.725, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.739, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.749, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Zn64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.857, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Zn66_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn66", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.909, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Zn68_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn68", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.917, + "uncertainty": null + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_nuclear_polarization_Zn70_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn70", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 0.973, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/shera_systematics_1976/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/shera_systematics_1976/Muonic Transition Energy Difference (different nuclides).json new file mode 100644 index 0000000..4754e8e --- /dev/null +++ b/radbase/compilation/shera_systematics_1976/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,1682 @@ +{ + "shera_systematics_1976_muonic_difference_Fe57_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe57", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.436, + "uncertainty": 0.05 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Fe56_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe56", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 2.2569, + "uncertainty": 0.0033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Fe56_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe56", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.133, + "uncertainty": 0.038 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Fe54_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe54", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 5.526, + "uncertainty": 0.038 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Fe54_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe54", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 4.09, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Fe54_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Fe54", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 2.957, + "uncertainty": 0.031 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Co59_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Co59", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 86.976, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Co59_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Co59", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 85.54, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Co59_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Co59", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 84.407, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Co59_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Co59", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 81.45, + "uncertainty": 0.048 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni64_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni64", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 170.745, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni64_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni64", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 169.309, + "uncertainty": 0.057 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni64_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni64", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 168.175, + "uncertainty": 0.05 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni64_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni64", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 165.218, + "uncertainty": 0.059 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni64_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni64", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 83.769, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.345, + "uncertainty": 0.056 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 170.908, + "uncertainty": 0.052 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 169.775, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 166.818, + "uncertainty": 0.055 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 85.368, + "uncertainty": 0.041 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni62_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni62", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.6, + "uncertainty": 0.029 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 173.909, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.473, + "uncertainty": 0.057 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 171.339, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 168.382, + "uncertainty": 0.006 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 86.933, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 3.164, + "uncertainty": 0.046 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni61_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni61", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.564, + "uncertainty": 0.041 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 174.884, + "uncertainty": 0.052 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 173.448, + "uncertainty": 0.048 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.315, + "uncertainty": 0.04 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 169.358, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 87.908, + "uncertainty": 0.035 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 4.14, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 2.54, + "uncertainty": 0.026 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni60_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni60", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 0.976, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 178.079, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 176.643, + "uncertainty": 0.042 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 175.51, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.553, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 91.103, + "uncertainty": 0.034 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 7.334, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 5.734, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 4.17, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Ni58_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Ni58", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 3.195, + "uncertainty": 0.031 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 258.031, + "uncertainty": 0.062 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 256.595, + "uncertainty": 0.058 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 255.462, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 252.505, + "uncertainty": 0.06 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 171.055, + "uncertainty": 0.048 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 87.286, + "uncertainty": 0.031 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 85.686, + "uncertainty": 0.031 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 84.122, + "uncertainty": 0.048 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 83.147, + "uncertainty": 0.035 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 252.949, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 258.512, + "uncertainty": 0.057 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 257.379, + "uncertainty": 0.05 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 254.422, + "uncertainty": 0.059 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.972, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 89.204, + "uncertainty": 0.037 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 87.604, + "uncertainty": 0.029 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 86.04, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 85.064, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 342.413, + "uncertainty": 0.121 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 340.977, + "uncertainty": 0.119 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 339.844, + "uncertainty": 0.116 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 255.437, + "uncertainty": 0.114 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 171.668, + "uncertainty": 0.112 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 170.068, + "uncertainty": 0.11 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 168.504, + "uncertainty": 0.115 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 167.529, + "uncertainty": 0.104 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 344.278, + "uncertainty": 0.062 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 342.842, + "uncertainty": 0.058 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 341.709, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 338.752, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 257.302, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 173.533, + "uncertainty": 0.038 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 171.934, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 170.369, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 169.394, + "uncertainty": 0.035 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 346.049, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 344.623, + "uncertainty": 0.058 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 343.49, + "uncertainty": 0.05 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 340.533, + "uncertainty": 0.06 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 259.083, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 175.315, + "uncertainty": 0.032 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 173.715, + "uncertainty": 0.03 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 172.151, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 171.175, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 348.234, + "uncertainty": 0.061 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 346.797, + "uncertainty": 0.057 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 345.664, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 342.707, + "uncertainty": 0.06 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 261.257, + "uncertainty": 0.048 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 177.489, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 175.489, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 174.325, + "uncertainty": 0.047 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 173.349, + "uncertainty": 0.034 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 336.887, + "uncertainty": 0.12 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu65_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu65", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 79.952, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 81.87, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Cu63_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Cu63", + "Nuclide_B": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 82.464, + "uncertainty": 0.112 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 164.334, + "uncertainty": 0.113 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 84.382, + "uncertainty": 0.111 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn70_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn70", + "Nuclide_B": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 82.464, + "uncertainty": 0.112 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 166.199, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 86.247, + "uncertainty": 0.038 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 84.33, + "uncertainty": 0.036 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn68_Zn70_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn68", + "Nuclide_B": "Zn70", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.865, + "uncertainty": 0.111 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 167.98, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 88.028, + "uncertainty": 0.033 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 86.111, + "uncertainty": 0.034 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Zn70_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Zn70", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 3.634, + "uncertainty": 0.111 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn66_Zn68_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn66", + "Nuclide_B": "Zn68", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.781, + "uncertainty": 0.026 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 170.155, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 90.203, + "uncertainty": 0.035 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 88.285, + "uncertainty": 0.031 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Zn70_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Zn70", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 5.821, + "uncertainty": 0.111 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Zn68_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Zn68", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 3.955, + "uncertainty": 0.027 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + }, + "shera_systematics_1976_muonic_difference_Zn64_Zn66_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide_A": "Zn64", + "Nuclide_B": "Zn66", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 2.174, + "uncertainty": 0.027 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting. Corrected for hyperfine splitting." + } +} diff --git a/radbase/compilation/shera_systematics_1976/Muonic Transition Energy.json b/radbase/compilation/shera_systematics_1976/Muonic Transition Energy.json new file mode 100644 index 0000000..24d2b95 --- /dev/null +++ b/radbase/compilation/shera_systematics_1976/Muonic Transition Energy.json @@ -0,0 +1,301 @@ +{ + "shera_systematics_1976_muonic_Fe54_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe54", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1255.849, + "uncertainty": 0.063 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Fe56_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe56", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1252.919, + "uncertainty": 0.058 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Fe57_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe57", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1251.823, + "uncertainty": 0.073 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Fe58_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe58", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1250.381, + "uncertainty": 0.067 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Co59_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Co59", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1336.553, + "uncertainty": 0.065 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Ni58_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni58", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1427.112, + "uncertainty": 0.06 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Ni60_2p1/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni60", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1423.86, + "uncertainty": 0.058 + }, + "Notes": "" + }, + "shera_systematics_1976_muonic_Fe54_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe54", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1260.011, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Fe56_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe56", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1257.054, + "uncertainty": 0.042 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Fe57_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe57", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1255.921, + "uncertainty": 0.051 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Fe58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Fe58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1254.485, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Co59_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Co59", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1341.461, + "uncertainty": 0.046 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Ni58_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni58", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1432.564, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Ni60_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni60", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1429.369, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Ni61_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni61", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1428.393, + "uncertainty": 0.049 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Ni62_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni62", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1426.829, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Ni64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Ni64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1425.229, + "uncertainty": 0.046 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Cu63_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Cu63", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1514.433, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Cu65_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Cu65", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1512.516, + "uncertainty": 0.045 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Zn64_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn64", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1602.718, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Zn66_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn66", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1600.544, + "uncertainty": 0.043 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Zn68_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn68", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1598.763, + "uncertainty": 0.044 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + }, + "shera_systematics_1976_muonic_Zn70_2p3/2_1s1/2": { + "Reference": "shera_systematics_1976", + "Nuclide": "Zn70", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 1596.898, + "uncertainty": 0.109 + }, + "Notes": "Combined Ka1 and Ka2 using theoretical FS splitting." + } +} diff --git a/radbase/compilation/test_test_1700/Calculated Muonic Nuclear Polarization.json b/radbase/compilation/test_test_1700/Calculated Muonic Nuclear Polarization.json new file mode 100644 index 0000000..531e671 --- /dev/null +++ b/radbase/compilation/test_test_1700/Calculated Muonic Nuclear Polarization.json @@ -0,0 +1,22 @@ +{ + "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2": { + "Reference": "test_test_1700", + "Nuclide": "Sn112", + "Level": "1s1/2", + "Energy [keV]": { + "value": 1755.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2": { + "Reference": "test_test_1700", + "Nuclide": "Sn112", + "Level": "2p1/2", + "Energy [keV]": { + "value": 255.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Radius.json b/radbase/compilation/test_test_1700/Muonic Radius.json new file mode 100644 index 0000000..e0439d9 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Radius.json @@ -0,0 +1,43 @@ +{ + "test_test_1700_radius_Pb203_NP_Vary": { + "Reference": "test_test_1700", + "Relies On": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2" + ], + "Nuclide": "Pb203", + "R [fm]": { + "value": 100.0, + "uncertainty": null + }, + "Nuclear Polarization Method": "Vary", + "Transition_A": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]_A": { + "value": 300.3, + "uncertainty": 0.3 + }, + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "test_test_1700_radius_Pb204_NP_Calculated": { + "Reference": "test_test_1700", + "Relies On": [ + "test_test_1700_muonic_Sn112_2p1/2_1s1/2" + ], + "Nuclide": "Pb204", + "R [fm]": { + "value": 100.3, + "uncertainty": 0.3 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [ + "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", + "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2" + ], + "Reduced Chi-Squared": 0.0, + "Notes": "" + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different nuclides).json new file mode 100644 index 0000000..4598b17 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,30 @@ +{ + "test_test_1700_muonic_difference_Fe1_Fe3_2p3/2_1s1/2": { + "Reference": "test_test_1700", + "Nuclide_A": "Fe1", + "Nuclide_B": "Fe3", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 1.0, + "uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonic_difference_Fe2_Fe4_2p3/2_1s1/2": { + "Reference": "test_test_1700", + "Nuclide_A": "Fe2", + "Nuclide_B": "Fe4", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 2.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy.json b/radbase/compilation/test_test_1700/Muonic Transition Energy.json index f527937..6696b99 100644 --- a/radbase/compilation/test_test_1700/Muonic Transition Energy.json +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy.json @@ -1,109 +1,14 @@ { - "test_test_1700_muonic_Pb204_2p_1s": { + "test_test_1700_muonic_Sn112_2p1/2_1s1/2": { "Reference": "test_test_1700", - "Nuclide": "Pb204", + "Nuclide": "Sn112", "Transition": { - "Upper": "2p", - "Lower": "1s" + "Upper": "2p1/2", + "Lower": "1s1/2" }, "Energy [keV]": { - "value": 300.0, - "uncertainty": null - }, - "Composite?": "No", - "Notes": "" - }, - "test_test_1700_muonic_Pb203_3p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb203", - "Transition": { - "Upper": "3p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 200.0, - "uncertainty": null - }, - "Composite?": "No", - "Notes": "" - }, - "test_test_1700_muonic_Pb203_2p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb203", - "Transition": { - "Upper": "2p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 100.0, - "uncertainty": null - }, - "Composite?": "No", - "Notes": "" - }, - "test_test_1700_muonic_Pb204_3p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb204", - "Transition": { - "Upper": "3p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 400.0, - "uncertainty": null - }, - "Composite?": "No", - "Notes": "" - }, - "test_test_1700_muonic_Pb200_2p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb200", - "Transition": { - "Upper": "2p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 202.0, - "uncertainty": null - }, - "Notes": "" - }, - "test_test_1700_muonic_Pb200_3p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb200", - "Transition": { - "Upper": "3p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 203.0, - "uncertainty": null - }, - "Notes": "" - }, - "test_test_1700_muonic_Pb100_2p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb100", - "Transition": { - "Upper": "2p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 102.0, - "uncertainty": null - }, - "Notes": "" - }, - "test_test_1700_muonic_Pb100_3p_1s": { - "Reference": "test_test_1700", - "Nuclide": "Pb100", - "Transition": { - "Upper": "3p", - "Lower": "1s" - }, - "Energy [keV]": { - "value": 103.0, - "uncertainty": null + "value": 3432.564, + "uncertainty": 0.06 }, "Notes": "" } diff --git a/radbase/data_entry.py b/radbase/data_entry.py index 0dc66f1..9b9d8f1 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -34,6 +34,28 @@ class Reference: doi: Optional[str] = None +class ScrollableFrame(ttk.Frame): + def __init__(self, container, *args, **kwargs): + super().__init__(container, *args, **kwargs) + canvas = tk.Canvas(self) + scrollbar = ttk.Scrollbar(self, orient="vertical", command=canvas.yview) + self.scrollable_frame = ttk.Frame(canvas) + + self.scrollable_frame.bind( + "", + lambda e: canvas.configure( + scrollregion=canvas.bbox("all") + ) + ) + + canvas.create_window((0, 0), window=self.scrollable_frame, anchor="nw") + + canvas.configure(yscrollcommand=scrollbar.set) + + canvas.pack(side="left", fill="both", expand=True) + scrollbar.pack(side="right", fill="y") + + class ToolTip: def __init__(self, widget, text: str, delay: int = 500): self.widget = widget @@ -81,13 +103,14 @@ def _hide(self, _=None): class FieldProcessor(Protocol): - def process(self, widget: tk.Widget) -> Any: + def process(self, widget: tk.Widget) -> dict[str, Any]: pass class CastProcessor: - def __init__(self, field_type: type, allows_empty: bool = False): + def __init__(self, field_type: type, key: str, allows_empty: bool = False): + self.key = key self.field_type = field_type self.allows_empty = allows_empty @@ -95,27 +118,124 @@ def process(self, widget: tk.Widget): raw = widget.get() if raw == "" and not self.allows_empty: raise ValueError("Field is empty") - return self.field_type(raw) + return {self.key: self.field_type(raw)} + + +class GroupedProcessor: + + def __init__(self, processors: list[FieldProcessor]): + self.processors = processors + + def process(self, widget: tk.Widget, allows_empty=False): + result = {} + + for sub_widget, processor in zip(widget.widgets, self.processors): + try: + sub_result = processor.process(sub_widget) + except ValueError: + continue + + result = result | sub_result + + if result == {} and not allows_empty: + raise ValueError(f'At least one sub_widget of {widget} must be non-empty for GroupedProcessor') + + return result + + +class XORProcessor: + # Requires exactly one of the two fields to be filled, and then returns data from filled out field. + def __init__(self, processors: list[FieldProcessor]): + self.processors = processors + + def process(self, widget: tk.Widget): + result = {} + + if len(widget.widgets) != 2: + raise ValueError('XOR processor applied to widget that does not have two fields.') + + num_filled = 0 + for sub_widget, processor in zip(widget.widgets, self.processors): + try: + sub_result = processor.process(sub_widget) + except ValueError: + continue + + num_filled += 1 + result = result | sub_result + + if num_filled != 1: + raise ValueError(f'Exactly one of the XOR fields must be filled, {num_filled} were filled.') + + return result class NumberWithUncertaintyProcessor: - @staticmethod - def process(widget: tk.Widget): + def __init__(self, key: str): + self.key = key + + def process(self, widget: tk.Widget): raw = widget.get().strip() try: value = float(raw) - return {'value': value, 'uncertainty': None} + return {self.key: {'value': value, 'uncertainty': None}} except ValueError: try: uvar = uncertainties.ufloat_fromstr(raw) - return {'value': uvar.n, 'uncertainty': uvar.s} + return {self.key: {'value': uvar.n, 'uncertainty': uvar.s}} except ValueError: raise ValueError( f'Entered value of {raw} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') +class NuclearPolarizationProcessor: + + @staticmethod + def process(widget: tk.Widget): + selection = widget.selection + fit_widget = widget.fit_widget + prev_calced_widget = widget.prev_calced_widget + + calced_processor = PreviousDataProcessor(key='Calculated Nuclear Polarization') + varied_processor = VariableNumberProcessor( + GroupedProcessor([ + XORProcessor( + [TransitionProcessor(), CastProcessor(str, key='Level')] + ), + NumberWithUncertaintyProcessor('Energy [keV]') + ])) + + mode = selection.get() + result = {'Nuclear Polarization Method': mode} + + if mode == 'Calculated': + return result | calced_processor.process(prev_calced_widget) + elif mode == 'Vary': + return result | varied_processor.process(fit_widget) + elif mode == 'Mixed': + return result | calced_processor.process(prev_calced_widget) | varied_processor.process(fit_widget) + else: + raise ValueError(f'{mode} is not in [Calculated, Vary, Mixed]') + + +class VariableNumberProcessor: + + def __init__(self, processor: FieldProcessor, suffixes: list[str] | None = None): + self.processor = processor + self.suffixes = suffixes if suffixes else [f'_{chr(ord('A') + i)}' for i in range(26)] + + def process(self, widget: tk.Widget) -> dict: + data = {} + for suffix, (label, widget) in zip(self.suffixes, widget.entries): + sub_result = self.processor.process(widget) + sub_result = {key + suffix: value for key, value in sub_result.items()} + data = data | sub_result + return data + + class MultiTransitionProcessor: + @staticmethod def process(widget: tk.Widget): data = {} @@ -125,20 +245,35 @@ def process(widget: tk.Widget): class NuclideProcessor: - @staticmethod - def process(widget: tk.Widget): + + def __init__(self, key: str = 'Nuclide'): + self.key = key + + def process(self, widget: tk.Widget): raw = widget.get() - if re.match(r'[a-zA-Z]{2}\d{1,3}', raw): - return raw - elif re.match(r'[a-zA-Z]{2}nat', raw): - return raw + if re.match(r'[a-zA-Z]{2}\d{1,3}', raw) or re.match(r'[a-zA-Z]{2}nat', raw): + return {self.key: raw} else: raise ValueError( 'Entered Nuclide does not match pattern of two letters and one to three numbers (Ex. Pb208') +class PreviousDataProcessor: + def __init__(self, key: str = 'Relies On'): + self.key = key + + def process(self, widget: tk.Widget) -> dict[str, list[str]]: + selected = [ + key + for key, var in widget.selection_vars.items() + if var.get() + ] + return {self.key: selected} + + class ReferenceProcessor: - def __init__(self, reference_path: Traversable): + def __init__(self, reference_path: Traversable, key: str = 'Reference'): + self.key = key self.reference_path = reference_path @property @@ -158,14 +293,15 @@ def process(self, widget: tk.Widget): f"Reference '{value}' is not a known citation key" ) - return value + return {self.key: value} class SelectProcessor: - def __init__(self, options: list[str]): + def __init__(self, options: list[str], key: str): + self.key = key self.options = set(options) - def process(self, widget: tk.Widget) -> str: + def process(self, widget: tk.Widget) -> dict[str, str]: value = widget.get().strip() if not value: @@ -174,7 +310,7 @@ def process(self, widget: tk.Widget) -> str: if value not in self.options: raise ValueError(f"'{value}' is not a valid selection") - return value + return {self.key: value} class TransitionProcessor: @@ -192,17 +328,19 @@ class TransitionProcessor: HYBRID_LEVEL_PATTERN = re.compile( r""" ^ - \d+[+-] # nuclear spin/parity (e.g. 2+, 0-) - , + (\d+[+-],)? # nuclear spin/parity (e.g. 2+, 0-) \d+ # principal quantum number [spdf] # orbital - \d+/\d+ # required j + \d/\d # required j $ """, re.VERBOSE ) - def process(self, widget: tk.Widget) -> dict[str, str]: + def __init__(self, key: str = 'Transition'): + self.key = key + + def process(self, widget: tk.Widget) -> dict[str, dict[str, str]]: upper = widget.upper_entry.get().strip() lower = widget.lower_entry.get().strip() @@ -217,7 +355,7 @@ def process(self, widget: tk.Widget) -> dict[str, str]: # both simple or both hybrid if upper_simple and lower_simple or upper_hybrid and lower_hybrid: - return {'Upper': upper, 'Lower': lower} + return {self.key: {'Upper': upper, 'Lower': lower}} raise ValueError( "Invalid transition format.\n" @@ -227,25 +365,12 @@ def process(self, widget: tk.Widget) -> dict[str, str]: ) -class PreviousMeasurementProcessor: - @staticmethod - def process(widget: tk.Widget) -> list[str]: - selected = [ - key - for key, var in widget.selection_vars.items() - if var.get() - ] - if not selected: - raise ValueError("At least one previous measurement must be selected") - return selected - - -class Widgetcreator(Protocol): +class WidgetCreator(Protocol): def create_widget(self, frame, row) -> tk.Widget: pass -class DefaultWidgetcreator: +class DefaultWidgetCreator: @staticmethod def create_widget(frame, row) -> tk.Widget: entry = ttk.Entry(frame, width=40) @@ -253,7 +378,131 @@ def create_widget(frame, row) -> tk.Widget: return entry -class PreviousMeasurementWidgetCreator: +class GroupedWidgetCreator: + + def __init__(self, labels: list[str], widget_creators: list[WidgetCreator]): + self.labels = labels + self.widget_creators = widget_creators + self.widgets = [] + + def create_widget(self, frame, row) -> tk.Widget: + grouped_frame = tk.Frame(frame) + grouped_frame.grid(row=row, column=1, pady=4, sticky='w') + grouped_frame.widgets = [] + + for i, (label, widget_creator) in enumerate(zip(self.labels, self.widget_creators)): + tk.Label(grouped_frame, text=label).grid(row=i, column=0, pady=4, sticky='w') + grouped_frame.widgets.append(widget_creator.create_widget(grouped_frame, i)) + + return grouped_frame + + +class NuclearPolarizationWidgetCreator: + + def __init__(self, compilation_path: Traversable): + self.compilation_path = compilation_path + + def create_widget(self, frame, row) -> tk.Widget: + container = ttk.Frame(frame) + container.grid(row=row, column=1, sticky="w") + + # Selection combobox (Calculated / Vary / Mixed) + selection = SelectWidgetCreator( + ["Calculated", "Vary", "Mixed"] + ).create_widget(container, row=0) + selection.grid(row=0, column=0, sticky="w", pady=4) + + # Sub-widgets + prev_calced_widget = PreviousDataWidgetCreator( + self.compilation_path, + filter_regex="muonic_nuclear" + ).create_widget(container, row=1) + + pair = GroupedWidgetCreator(['', 'Energy [keV]'], [GroupedWidgetCreator(['Transition', 'Level'], + [TransitionWidgetCreator(), + DefaultWidgetCreator()]), + DefaultWidgetCreator()]) + fit_widget = VariableNumberWidgetCreator(pair).create_widget(container, row=1) + + # Start hidden + prev_calced_widget.grid_remove() + fit_widget.grid_remove() + + def handle_selection(event=None): + mode = selection.get() + + if mode == "Calculated": + prev_calced_widget.grid(row=1, column=0) + fit_widget.grid_remove() + + elif mode == "Vary": + prev_calced_widget.grid_remove() + fit_widget.grid(row=1, column=0) + + elif mode == "Mixed": + prev_calced_widget.grid(row=1, column=0) + fit_widget.grid(row=2, column=0) + + selection.bind("<>", handle_selection) + handle_selection() + + container.selection = selection + container.fit_widget = fit_widget + container.prev_calced_widget = prev_calced_widget + return container + + +class VariableNumberWidgetCreator: + + def __init__(self, widget_creator: WidgetCreator): + self.widget_creator = widget_creator + + def create_widget(self, frame, row): + + class MultiContainer(ttk.Frame): # Mainly for type hinting + def __init__(self, entries, buttons, *args, **kwargs): + super().__init__(frame, *args, **kwargs) + self.entries: list[tuple[tk.Label, tk.Widget]] = entries + self.buttons: list[tk.Button] = buttons + + def regrid(self): + for i, (label, entry) in enumerate(self.entries): + label.grid(row=i), entry.grid(row=i) + for button in self.buttons: + button.grid(row=len(self.entries)) + + container = MultiContainer(entries=[], buttons=[]) + container.grid(row=row, column=1, pady=4, sticky="w") + + def add_new_entry(*_): + number_of_rows = len(container.entries) + new_letter = f'{chr(ord("A") + number_of_rows)}' + + label = tk.Label(container, text=f'{new_letter}') + label.grid(row=number_of_rows, column=0) + + next_entry = self.widget_creator.create_widget(frame=container, row=number_of_rows) + + container.entries.append((label, next_entry)) + container.regrid() + + def delete_entry(*_): + label, entry = container.entries.pop() + label.grid_forget(), entry.grid_forget() + container.regrid() + + add_button = ttk.Button(container, text="Add", command=add_new_entry, takefocus=0) + add_button.grid(row=0, column=0, pady=10) + + delete_button = ttk.Button(container, text="Remove", command=delete_entry, takefocus=0) + delete_button.grid(row=0, column=1, pady=10) + container.buttons = [add_button, delete_button] + add_new_entry(), add_new_entry() + + return container + + +class PreviousDataWidgetCreator: def __init__(self, compilation_path: Traversable, filter_regex: str = ""): self.filter_regex = filter_regex @@ -273,7 +522,6 @@ def load_previous_measurements_from_json(compilation_path: Traversable) -> list[ return sorted(previous_measurements) - # CHATGPT generated. TODO: Double check this works as intended. def create_widget(self, frame, row) -> tk.Widget: container = ttk.Frame(frame) container.grid(row=row, column=1, pady=4, sticky="w") @@ -633,9 +881,9 @@ def delete_transition(*_): class FieldSpec(NamedTuple): - name: str + label: str processor: FieldProcessor - widget_creator: Widgetcreator = DefaultWidgetcreator() + widget_creator: WidgetCreator = DefaultWidgetCreator() hovertext: str | None = None @@ -654,7 +902,13 @@ class InputTemplate(NamedTuple): transition_field = FieldSpec("Transition", TransitionProcessor(), TransitionWidgetCreator(), hovertext='Enter the upper and lower levels of the atomic/muonic transition') -notes_field = FieldSpec("Notes", CastProcessor(str, allows_empty=True)) +transition_or_level_field = FieldSpec("Transition\nor Level", + XORProcessor([TransitionProcessor(), CastProcessor(str, key='Level')]), + GroupedWidgetCreator(['Transition', 'Level'], + [TransitionWidgetCreator(), DefaultWidgetCreator()]), + hovertext='The transition/level for which the nuclear polarization calculation was done.') + +notes_field = FieldSpec("Notes", CastProcessor(str, key='Notes', allows_empty=True)) # LIST TEMPLATES HERE. Each template must include a FieldSpec named "Reference". muonic_transition_energy_template = InputTemplate( @@ -663,7 +917,7 @@ class InputTemplate(NamedTuple): reference_field, nuclide_field, transition_field, - FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor()), + FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor("Energy [keV]")), notes_field ], data_key=lambda values: '_'.join([values['Reference'], 'muonic', values['Nuclide'], @@ -673,14 +927,14 @@ class InputTemplate(NamedTuple): name="Muonic Transition Energy Difference (different nuclides)", fields=[ reference_field, - FieldSpec("Nuclide A", NuclideProcessor()), - FieldSpec("Nuclide B", NuclideProcessor()), + FieldSpec("Nuclide A", NuclideProcessor(key="Nuclide_A")), + FieldSpec("Nuclide B", NuclideProcessor(key="Nuclide_B")), transition_field, - FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor("Energy Difference [keV] (A-B)")), notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'muonic_difference', values['NuclideA'], values['NuclideB'], + [values['Reference'], 'muonic_difference', values['Nuclide_A'], values['Nuclide_B'], values['Transition']['Upper'], values['Transition']['Lower']]) ) @@ -689,28 +943,55 @@ class InputTemplate(NamedTuple): fields=[ reference_field, nuclide_field, - FieldSpec("Transitions", MultiTransitionProcessor(), MultiTransitionWidgetCreator(), + FieldSpec("Transitions", MultiTransitionProcessor(), VariableNumberWidgetCreator(TransitionWidgetCreator()), hovertext='Enter the upper and lower levels of the atomic/muonic transition'), - FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor()), + FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor("Energy Difference [keV] (A-B)")), notes_field ], data_key=lambda values: '_'.join( [values['Reference'], 'muonic_difference', values['Nuclide'], - *list(sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values['Transitions'].items()], ()))]) + *list( + sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values['Transitions'].items()], + ()))]) ) + +def mu_nuc_pol_key(values): + if 'Transition' in values: + return '_'.join([values['Reference'], 'muonic_nuclear_polarization', values['Nuclide'], + values['Transition']['Upper'], values['Transition']['Lower']]) + else: + return '_'.join([values['Reference'], 'muonic_nuclear_polarization', values['Nuclide'], + values['Level']]) + + +muonic_nuclear_polarization_calculation_template = InputTemplate( + name="Calculated Muonic Nuclear Polarization", + fields=[ + reference_field, + nuclide_field, + transition_or_level_field, + FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor("Energy [keV]")), + notes_field + ], + data_key=mu_nuc_pol_key) + muonic_barret_theory_template = InputTemplate( name="Muonic Barrett Moment", fields=[ reference_field, - FieldSpec("Data used as input", PreviousMeasurementProcessor(), - PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], - filter_regex='muonic.*_')), + FieldSpec("Data used as input", PreviousDataProcessor(), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), nuclide_field, - FieldSpec('Rka [fm]', NumberWithUncertaintyProcessor()), - FieldSpec('k [-]', CastProcessor(str)), - FieldSpec('alpha [1/fm]', CastProcessor(str)), - FieldSpec('Cz [fm/keV]', CastProcessor(str)), + FieldSpec('Rka [fm]', NumberWithUncertaintyProcessor('Rka [fm]')), + FieldSpec('k [-]', CastProcessor(str, key='k [-]')), + FieldSpec('alpha [1/fm]', CastProcessor(str, key='alpha [1/fm]')), + FieldSpec('Cz [fm/keV]', CastProcessor(str, key='Cz [fm/keV]')), + FieldSpec('Nuclear Polarization Method', + NuclearPolarizationProcessor(), + NuclearPolarizationWidgetCreator(compilation_path=config['compilation_dir']), + hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), notes_field ], data_key=lambda values: '_'.join([values['Reference'], 'barrett_moment', values['Nuclide'], @@ -722,15 +1003,16 @@ class InputTemplate(NamedTuple): name="Muonic Radius", fields=[ reference_field, - FieldSpec("Data used as input", PreviousMeasurementProcessor(), - PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], - filter_regex='muonic.*_')), + FieldSpec("Data used as input", PreviousDataProcessor(), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), nuclide_field, - FieldSpec('R [fm]', NumberWithUncertaintyProcessor()), - FieldSpec('Nuclear Polarization Method', SelectProcessor(['Calculated', 'Fit']), - SelectWidgetCreator(['Calculated', 'Fit']), + FieldSpec('R [fm]', NumberWithUncertaintyProcessor(key='R [fm]')), + FieldSpec('Nuclear Polarization Method', + NuclearPolarizationProcessor(), + NuclearPolarizationWidgetCreator(compilation_path=config['compilation_dir']), hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), - FieldSpec('Reduced Chi-Squared', CastProcessor(float, allows_empty=True)), + FieldSpec('Reduced Chi-Squared', CastProcessor(float, key='Reduced Chi-Squared', allows_empty=True)), notes_field ], data_key=lambda values: '_'.join([values['Reference'], 'radius', values['Nuclide'], @@ -741,13 +1023,15 @@ class InputTemplate(NamedTuple): name="Fermi Distribution", fields=[ reference_field, - FieldSpec("Data used as input", PreviousMeasurementProcessor(), - PreviousMeasurementWidgetCreator(compilation_path=config['compilation_dir'], - filter_regex='muonic.*_')), + FieldSpec("Data used as input", PreviousDataProcessor(), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), nuclide_field, # TODO add fermi distribution processor and widget creator with different fermi distribution options. - FieldSpec('c [fm]', NumberWithUncertaintyProcessor()), - FieldSpec('a [fm]', NumberWithUncertaintyProcessor()), + FieldSpec('c [fm]', NumberWithUncertaintyProcessor(key='c [fm]')), + FieldSpec('a [fm]', NumberWithUncertaintyProcessor(key='a [fm]')), + FieldSpec('beta2 [-]', NumberWithUncertaintyProcessor(key='beta2 [-]')), + FieldSpec('beta4 [-]', NumberWithUncertaintyProcessor(key='beta4 [-]')), notes_field ], data_key=lambda values: '_'.join([values['Reference'], 'fermi', values['Nuclide']]) @@ -756,6 +1040,7 @@ class InputTemplate(NamedTuple): templates = [muonic_transition_energy_template, muonic_transition_energy_difference_template, muonic_transition_energy_difference_diff_transition_template, + muonic_nuclear_polarization_calculation_template, muonic_barret_theory_template, muonic_radius_template, muonic_fermi_distribution_template] @@ -796,6 +1081,7 @@ def __init__(self, if start_interface: self.root = tk.Tk() + self.root.geometry("600x500") self.root.title("Data Entry Interface") def _on_mousewheel(event): @@ -873,12 +1159,14 @@ def display_input(self, template: InputTemplate): wraplength=300 ).pack(pady=10) - form_frame = ttk.Frame(self.root) - form_frame.pack(padx=10, pady=10, fill="x") + form_frame = ScrollableFrame(self.root) + form_frame.pack(padx=10, pady=10, expand=True, fill='both') + + form_frame = form_frame.scrollable_frame for row, field in enumerate(template.fields): label = ttk.Label(form_frame, - text=field.name, + text=field.label, font=("Arial", 11), wraplength=120 ) @@ -887,10 +1175,10 @@ def display_input(self, template: InputTemplate): ToolTip(label, field.hovertext) entry = field.widget_creator.create_widget(form_frame, row) - self.current_entries[field.name] = (entry, field.processor) + self.current_entries[field.label] = (entry, field.processor) keep_var = tk.BooleanVar(value=False) - self.keep_vars[field.name] = keep_var + self.keep_vars[field.label] = keep_var keep_check = ttk.Checkbutton( form_frame, @@ -943,7 +1231,7 @@ def select_for_twod_input(self, template): justify="left" ).pack(padx=20, pady=15) - field_names = [field.name for field in template.fields] + field_names = [field.label for field in template.fields] btn_frame = ttk.Frame(dialog) btn_frame.pack(fill="both", expand=True, padx=20, pady=10) buttons = [] @@ -992,7 +1280,8 @@ def twod_input(self, template, row_field, col_field, value_field): main_btn_frame = ttk.Frame(frame) main_btn_frame.grid(row=0, column=0, sticky='w') tk.Button(main_btn_frame, text='Submit', - command=lambda: self.submit_2d(template, row_field, col_field, value_field, row_widgets, col_widgets, cells)).pack() + command=lambda: self.submit_2d(template, row_field, col_field, value_field, row_widgets, col_widgets, + cells)).pack() tk.Button(main_btn_frame, text='Back', command=lambda: dialog.destroy()).pack() row_widgets: list[tk.Widget] = [] @@ -1000,8 +1289,10 @@ def twod_input(self, template, row_field, col_field, value_field): cells: list[list[tk.Widget]] = [] def make_widget(field_name): - field, = [field for field in template.fields if field.name == field_name] - return field.widget_creator.create_widget(grid_frame, row=0) + field, = [field for field in template.fields if field.label == field_name] + widget = field.widget_creator.create_widget(grid_frame, row=0) + widget.config(width=20) + return widget def regrid(): for w in grid_frame.winfo_children(): @@ -1060,16 +1351,26 @@ def submit_2d(self, template, row_field, col_field, value_field, row_widgets, co # We take each (row_widget, col_widget, cell_widget) triplet, fill them in to the main data entry tab, # and trigger the data submission. - original_entries = {field_name: self.current_entries[field_name] for field_name in (row_field, col_field, value_field)} + original_entries = {field_name: self.current_entries[field_name] for field_name in + (row_field, col_field, value_field)} for row_widget, cell_row in zip(row_widgets, cells): for col_widget, cell in zip(col_widgets, cell_row): + + try: + if not cell.get(): + continue + except AttributeError: + continue + for field_name, widget in [(row_field, row_widget), (col_field, col_widget), (value_field, cell)]: prev_entry, processor = self.current_entries[field_name] self.current_entries[field_name] = (widget, processor) - self.submit_data(template, clear_fields=False) # We don't want to erase our row/col entries as we submit + self.submit_data(template, + clear_fields=False) # We don't want to erase our row/col entries as we submit - for field_name in (row_field, col_field, value_field): # make sure we restore the original widgets once we are done submitting. + for field_name in (row_field, col_field, + value_field): # make sure we restore the original widgets once we are done submitting. self.current_entries[field_name] = original_entries[field_name] pass @@ -1090,7 +1391,12 @@ def clear_widget(widg: tk.Widget): try: for field_name, (widget, processor) in self.current_entries.items(): - data[field_name] = processor.process(widget) + result = processor.process(widget) + if overlap := set(data.keys()).intersection(set(result.keys())): # Key collision + raise ValueError( + f'Tried to add {field_name} data, but {overlap} field(s) are already present from another widget') + data = data | result + except ValueError as e: messagebox.showerror("Invalid Input", str(e)) return diff --git a/radbase/startup/compare_to_angeli.py b/radbase/startup/compare_to_angeli.py index 594513c..791c4a3 100644 --- a/radbase/startup/compare_to_angeli.py +++ b/radbase/startup/compare_to_angeli.py @@ -45,7 +45,7 @@ def compare_rel_results(filename, rel1, rel2, lsuffix='x', rsuffix='y'): series = merge_df.iloc[:, col[0].column - 1] max_len = max(( series.astype(str).map(len).max(), # len of largest item - len(str(series.name)) # len of column name/header + len(str(series.label)) # len of column name/header )) + 1 # adding a little extra space) worksheet.column_dimensions[ openpyxl.utils.get_column_letter(col[0].column)].width = max_len # set column width @@ -95,7 +95,7 @@ def compare_abs_results(filename, absl1, absl2, lsuffix='x', rsuffix='y'): series = merge_df.iloc[:, col[0].column - 1] max_len = max(( series.astype(str).map(len).max(), # len of largest item - len(str(series.name)) # len of column name/header + len(str(series.label)) # len of column name/header )) + 1 # adding a little extra space) worksheet.column_dimensions[ openpyxl.utils.get_column_letter(col[0].column)].width = max_len # set column width diff --git a/readme.rst b/readme.rst index 12cd81b..22a9754 100644 --- a/readme.rst +++ b/readme.rst @@ -6,22 +6,27 @@ radbase Overview --------- -Created in preparation for the 2024 IAEA Technical Meeting on Compilation and Evaluation of Nuclear Charge Radii. +Created in preparation for the 2025 IAEA Technical Meeting on Compilation and Evaluation of Nuclear Charge Radii. -**This repostiory is in an alpha stage; all features/syntax are subject to change without notice.** +**This repostiory is in an alpha stage; all features/data/syntax are subject to change without notice.** Contains the following classes: -* ``RadiusDataMapper`` - A database of all nuclear radius related measurements and associated references (in-progress). + * ``RadiusAnalyzer`` - Flexible analysis via a non-linear least squares procedure (in-progress) * Built-in statistical outlier detection (not started) * Analyzes graph formed by data to reduce computational load (In progress) -* ``RadiusDataVisualizer`` - Interactive visualization of measurements and optimized radii (not started) +* ``RadiusDataVisualizer`` - Interactive visualization of measurements and optimized radii (in-progress) * Aids in visualizing: * Primary vs. Secondary nuclides * Number of measurements for each connection/nuclide * Coverage of individual labs + +* ``DataEntryVisualizer`` - User interface to enter nuclear radius data (in-progress) + + * Includes different templates for different kinds of information + * Fields include validation, dynamic resizing, and searches of previously entered data diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py index b05e137..3536626 100644 --- a/tests/test_data_entry.py +++ b/tests/test_data_entry.py @@ -1,18 +1,17 @@ import json -# Allows for import os -import pathlib -import tkinter as tk from tkinter import ttk import pytest from radbase.data_entry import (CastProcessor, DataEntryInterface, FieldSpec, - InputTemplate, NuclideProcessor, + GroupedProcessor, InputTemplate, + NuclideProcessor, NumberWithUncertaintyProcessor, - ReferenceProcessor, templates) + ReferenceProcessor, TransitionProcessor, + XORProcessor) -if os.environ.get('DISPLAY','') == '': +if os.environ.get('DISPLAY', '') == '': print('no display found. Using :0.0') os.environ.__setitem__('DISPLAY', ':0.0') @@ -34,8 +33,7 @@ 'Reference': list(example_references.keys())[0], 'Previous Muonic Measurements': list(example_references.keys())[0] + '_muonic_2p1/2_1s1/2', 'Nuclide': 'Pb208' - '' - + '' } @@ -49,11 +47,11 @@ def make_dummy_references(tmp_path): class DummyProcessor: @staticmethod def process(widget): - return 'nothing' + return {'test': 'nothing'} dummy_template = InputTemplate(name='test', - fields=[FieldSpec('Reference', CastProcessor(str)), + fields=[FieldSpec('Reference', CastProcessor(str, 'test')), FieldSpec('testfield', DummyProcessor())], data_key=lambda x: 'testkey') @@ -65,18 +63,21 @@ def __init__(self, value): def get(self): return self.value + def __str__(self): + return f'DummyWidget(={self.value})' + def test_cast_processor(): widget = DummyWidget('30.2') blank_widget = DummyWidget('') - assert CastProcessor(str).process(widget) == '30.2' - assert CastProcessor(float).process(widget) == 30.2 + assert CastProcessor(str, 'test').process(widget) == {'test': '30.2'} + assert CastProcessor(float, 'test').process(widget) == {'test': 30.2} with pytest.raises(ValueError) as e_info: # should raise error if it can not cast - CastProcessor(int).process(widget) + CastProcessor(int, '').process(widget) with pytest.raises(ValueError) as e_info: # should raise error if field was left blank. - CastProcessor(str).process(blank_widget) + CastProcessor(str, '').process(blank_widget) def test_nuclide_processor(): @@ -84,14 +85,13 @@ def test_nuclide_processor(): natwidget = DummyWidget('Pbnat') bad_widget = DummyWidget('082203') - assert NuclideProcessor().process(widget) == 'Pb208' - assert NuclideProcessor().process(natwidget) == 'Pbnat' + assert NuclideProcessor(key='Nuclide').process(widget) == {'Nuclide': 'Pb208'} + assert NuclideProcessor(key='Nuclide').process(natwidget) == {'Nuclide': 'Pbnat'} with pytest.raises(ValueError) as e_info: NuclideProcessor().process(bad_widget) def test_reference_processor(tmp_path): - global example_references good_widget = DummyWidget('Smith_nuclear_1978') @@ -100,25 +100,99 @@ def test_reference_processor(tmp_path): tmp_ref_path = make_dummy_references(tmp_path) ref_proc = ReferenceProcessor(tmp_ref_path) - assert ref_proc.process(good_widget) == 'Smith_nuclear_1978' + assert ref_proc.process(good_widget) == {'Reference': 'Smith_nuclear_1978'} with pytest.raises(ValueError) as e_info: ref_proc.process(bad_widget) def test_number_with_uncertainty_processor(): - float_widget = DummyWidget('100.1') uncertainty_widget = DummyWidget('100.1(3)') bad_widget = DummyWidget('bad') - ref_proc = NumberWithUncertaintyProcessor() + ref_proc = NumberWithUncertaintyProcessor('test') - assert ref_proc.process(float_widget) == {'value': 100.1, 'uncertainty': None} - assert ref_proc.process(uncertainty_widget) == {'value': 100.1, 'uncertainty': 0.3} + assert ref_proc.process(float_widget) == {'test': {'value': 100.1, 'uncertainty': None}} + assert ref_proc.process(uncertainty_widget) == {'test': {'value': 100.1, 'uncertainty': 0.3}} with pytest.raises(ValueError) as e_info: ref_proc.process(bad_widget) +def test_XOR_processor(): + xor_proc = XORProcessor([CastProcessor(str, key='label1'), CastProcessor(str, key='label2')]) + + parent_widget = DummyWidget(None) + filled_widget = DummyWidget('test') + empty_widget = DummyWidget('') + + parent_widget.widgets = [filled_widget, empty_widget] + assert xor_proc.process(parent_widget) == {'label1': 'test'} + + parent_widget.widgets = [empty_widget, filled_widget] + assert xor_proc.process(parent_widget) == {'label2': 'test'} + + parent_widget.widgets = [empty_widget, empty_widget] + with pytest.raises(ValueError) as e_info: + xor_proc.process(parent_widget) + + parent_widget.widgets = [filled_widget, filled_widget] + with pytest.raises(ValueError) as e_info: + xor_proc.process(parent_widget) + + +def test_grouped_processor(): + grouped_proc = GroupedProcessor([CastProcessor(str, key='label1'), CastProcessor(str, key='label2')]) + + parent_widget = DummyWidget(None) + filled_widget = DummyWidget('test') + empty_widget = DummyWidget('') + + parent_widget.widgets = [filled_widget, empty_widget] + assert grouped_proc.process(parent_widget) == {'label1': 'test'} + + parent_widget.widgets = [empty_widget, filled_widget] + assert grouped_proc.process(parent_widget) == {'label2': 'test'} + + parent_widget.widgets = [empty_widget, empty_widget] + with pytest.raises(ValueError) as e_info: + grouped_proc.process(parent_widget) + + parent_widget.widgets = [filled_widget, filled_widget] + assert grouped_proc.process(parent_widget) == {'label1': 'test', 'label2': 'test'} + + +def test_transition_processor(): + trans_widget = DummyWidget('') + + bad_level = DummyWidget('2pp') + + simple_upper = DummyWidget('2p') + simple_lower = DummyWidget('1s') + + withj_upper = DummyWidget('2p1/2') + withj_lower = DummyWidget('1s1/2') + + nuclear_upper = DummyWidget('2+,2p1/2') + nuclear_lower = DummyWidget('0+,1s1/2') + + trans_widget.upper_entry, trans_widget.lower_entry = simple_upper, simple_lower + assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2p', 'Lower': '1s'}} + + trans_widget.upper_entry, trans_widget.lower_entry = withj_upper, withj_lower + assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2p1/2', 'Lower': '1s1/2'}} + + trans_widget.upper_entry, trans_widget.lower_entry = nuclear_upper, nuclear_lower + assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2+,2p1/2', 'Lower': '0+,1s1/2'}} + + with pytest.raises(ValueError) as e_info: + trans_widget.upper_entry, trans_widget.lower_entry = bad_level, bad_level + TransitionProcessor().process(trans_widget) + + trans_widget.upper_entry, trans_widget.lower_entry = withj_upper, nuclear_lower + TransitionProcessor().process(trans_widget) + + + # def test_init_data_entry_interface(tmp_path): # # global example_references @@ -130,7 +204,6 @@ def test_number_with_uncertainty_processor(): def test_save_data(tmp_path): - ref_key = list(example_references.keys())[0] test_data = {'Reference': ref_key, 'testfield': 3} tmp_path.mkdir(exist_ok=True) @@ -149,7 +222,6 @@ def test_save_data(tmp_path): interface.save_data(dummy_template, test_data, replacement_strategy='NeverReplace') assert json.loads(tmp_data_loc.read_text()) == {'testkey': new_test_data} - # def test_previous_measurement_processor(tmp_path): # # previous_measurements = {'Authors'} From 528b7d99cae1dd2af638c26fd05eabf0b22020ee Mon Sep 17 00:00:00 2001 From: Hunter Date: Wed, 11 Feb 2026 15:11:20 -0500 Subject: [PATCH 05/11] HOTFIX: Different Transitions Template --- .../phan_nuclear_1985/Muonic Radius.json | 28 +++++++++++++++++++ .../Muonic Transition Energy.json | 15 ++++++++++ radbase/compilation/references.json | 17 +++++++++++ ...gy Difference (different transitions).json | 19 +++++++++++++ radbase/data_entry.py | 4 +-- 5 files changed, 81 insertions(+), 2 deletions(-) create mode 100644 radbase/compilation/phan_nuclear_1985/Muonic Radius.json create mode 100644 radbase/compilation/phan_nuclear_1985/Muonic Transition Energy.json create mode 100644 radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json diff --git a/radbase/compilation/phan_nuclear_1985/Muonic Radius.json b/radbase/compilation/phan_nuclear_1985/Muonic Radius.json new file mode 100644 index 0000000..f0fa2d8 --- /dev/null +++ b/radbase/compilation/phan_nuclear_1985/Muonic Radius.json @@ -0,0 +1,28 @@ +{ + "phan_nuclear_1985_radius_Zr90_NP_Mixed": { + "Reference": "phan_nuclear_1985", + "Relies On": [], + "Nuclide": "Zr90", + "R [fm]": { + "value": 4.2724, + "uncertainty": 0.0009 + }, + "Nuclear Polarization Method": "Mixed", + "Calculated Nuclear Polarization": [ + "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", + "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2" + ], + "Level_A": "1s", + "Energy [keV]_A": { + "value": 175.0, + "uncertainty": 22.0 + }, + "Level_B": "2s", + "Energy [keV]_B": { + "value": 175.0, + "uncertainty": 22.0 + }, + "Reduced Chi-Squared": 0.76, + "Notes": "" + } +} diff --git a/radbase/compilation/phan_nuclear_1985/Muonic Transition Energy.json b/radbase/compilation/phan_nuclear_1985/Muonic Transition Energy.json new file mode 100644 index 0000000..885b86a --- /dev/null +++ b/radbase/compilation/phan_nuclear_1985/Muonic Transition Energy.json @@ -0,0 +1,15 @@ +{ + "phan_nuclear_1985_muonic_Zr90_2s1/2_2p3/2": { + "Reference": "phan_nuclear_1985", + "Nuclide": "Zr90", + "Transition": { + "Upper": "2s1/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 106.404, + "uncertainty": 0.009 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json index 00faac5..298cf7e 100644 --- a/radbase/compilation/references.json +++ b/radbase/compilation/references.json @@ -155,5 +155,22 @@ "pages": "731-748", "url": "10.1103/PhysRevC.14.731", "doi": "https://link.aps.org/doi/10.1103/PhysRevC.14.731" + }, + "phan_nuclear_1985": { + "title": "Nuclear polarization in muonic 90Zr", + "author": [ + "T. Q. Phan", + "P. Bergem", + "A. R\u00fcetschi", + "L. A. Schaller", + "L. Schellenberg" + ], + "year": "1985", + "month": "August", + "journal": "Physical Review C", + "volume": "32", + "pages": "609-619", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.32.609", + "doi": "10.1103/PhysRevC.32.609" } } diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json new file mode 100644 index 0000000..80b4a75 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json @@ -0,0 +1,19 @@ +{ + "test_test_1700_muonic_difference_Zr90": { + "Reference": "test_test_1700", + "Nuclide": "Zr90", + "Transition_A": { + "Upper": "3p3/2", + "Lower": "1s1/2" + }, + "Transition_B": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy Difference [keV] (A-B)": { + "value": 100.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/data_entry.py b/radbase/data_entry.py index 9b9d8f1..f49a698 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -943,7 +943,7 @@ class InputTemplate(NamedTuple): fields=[ reference_field, nuclide_field, - FieldSpec("Transitions", MultiTransitionProcessor(), VariableNumberWidgetCreator(TransitionWidgetCreator()), + FieldSpec("Transitions", VariableNumberProcessor(TransitionProcessor()), VariableNumberWidgetCreator(TransitionWidgetCreator()), hovertext='Enter the upper and lower levels of the atomic/muonic transition'), FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor("Energy Difference [keV] (A-B)")), notes_field @@ -951,7 +951,7 @@ class InputTemplate(NamedTuple): data_key=lambda values: '_'.join( [values['Reference'], 'muonic_difference', values['Nuclide'], *list( - sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values['Transitions'].items()], + sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values.items() if 'Transition' in field_name.lower()], ()))]) ) From bad3876b1d785cf21d73399320992221cf54eb38 Mon Sep 17 00:00:00 2001 From: Hunter Date: Mon, 16 Feb 2026 13:27:57 -0500 Subject: [PATCH 06/11] Before added Wo81 --- .pre-commit-config.yaml | 2 +- radbase/compilation/__init__.py | 0 .../Fermi Distribution.json | 162 + ...nergy Difference (different nuclides).json | 57 + .../Muonic Transition Energy.json | 368 ++ .../hahn_experimental_1979/energies.txt | 7 + .../hahn_1979_process.py | 32 + .../hahn_experimental_1979/notes.txt | 4 + .../kast_isotone_1971/Fermi Distribution.json | 208 ++ .../kast_isotone_1971/Muonic Radius.json | 92 + .../Muonic Transition Energy.json | 314 ++ ...alculated Muonic Nuclear Polarization.json | 12 + radbase/compilation/references.json | 89 + .../saito_muonic_2025/Fermi Distribution.json | 110 + .../Muonic Barrett Moment.json | 467 +++ .../Muonic Transition Energy.json | 338 ++ .../compilation/saito_muonic_2025/notes.txt | 4 + .../saito_muonic_2025/saito_2025_process.py | 49 + .../compilation/saito_muonic_2025/values.txt | 28 + ...nergy Difference (different nuclides).json | 2956 +++++++++++++++++ .../wolfhahrt_nuclear_1981/energy_diffs.csv | 211 ++ .../wolfhart_1981_process.py | 36 + radbase/data_entry.py | 46 +- 23 files changed, 5584 insertions(+), 8 deletions(-) create mode 100644 radbase/compilation/__init__.py create mode 100644 radbase/compilation/hahn_experimental_1979/Fermi Distribution.json create mode 100644 radbase/compilation/hahn_experimental_1979/Muonic Transition Energy Difference (different nuclides).json create mode 100644 radbase/compilation/hahn_experimental_1979/Muonic Transition Energy.json create mode 100644 radbase/compilation/hahn_experimental_1979/energies.txt create mode 100644 radbase/compilation/hahn_experimental_1979/hahn_1979_process.py create mode 100644 radbase/compilation/hahn_experimental_1979/notes.txt create mode 100644 radbase/compilation/kast_isotone_1971/Fermi Distribution.json create mode 100644 radbase/compilation/kast_isotone_1971/Muonic Radius.json create mode 100644 radbase/compilation/kast_isotone_1971/Muonic Transition Energy.json create mode 100644 radbase/compilation/phan_nuclear_1985/Calculated Muonic Nuclear Polarization.json create mode 100644 radbase/compilation/saito_muonic_2025/Fermi Distribution.json create mode 100644 radbase/compilation/saito_muonic_2025/Muonic Barrett Moment.json create mode 100644 radbase/compilation/saito_muonic_2025/Muonic Transition Energy.json create mode 100644 radbase/compilation/saito_muonic_2025/notes.txt create mode 100644 radbase/compilation/saito_muonic_2025/saito_2025_process.py create mode 100644 radbase/compilation/saito_muonic_2025/values.txt create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py diff --git a/.pre-commit-config.yaml b/.pre-commit-config.yaml index 4a1baf6..438b97e 100644 --- a/.pre-commit-config.yaml +++ b/.pre-commit-config.yaml @@ -19,7 +19,7 @@ repos: hooks: - id: flake8 additional_dependencies: [flake8-deprecated, flake8-mutable, Flake8-pyproject] - exclude: tests/ + exclude: 'tests/.*|radbase/compilation/.*' - repo: https://github.com/PyCQA/isort/ rev: 5.13.2 diff --git a/radbase/compilation/__init__.py b/radbase/compilation/__init__.py new file mode 100644 index 0000000..e69de29 diff --git a/radbase/compilation/hahn_experimental_1979/Fermi Distribution.json b/radbase/compilation/hahn_experimental_1979/Fermi Distribution.json new file mode 100644 index 0000000..9ffc632 --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/Fermi Distribution.json @@ -0,0 +1,162 @@ +{ + "hahn_experimental_1979_fermi_Hg198": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2" + ], + "Nuclide": "Hg198", + "c [fm]": { + "value": 6.5712, + "uncertainty": 0.002 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + }, + "hahn_experimental_1979_fermi_Hg200": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2" + ], + "Nuclide": "Hg200", + "c [fm]": { + "value": 6.5829, + "uncertainty": 0.0023 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + }, + "hahn_experimental_1979_fermi_Hg202": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2" + ], + "Nuclide": "Hg202", + "c [fm]": { + "value": 6.5962, + "uncertainty": 0.0023 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + }, + "hahn_experimental_1979_fermi_Hg204": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2" + ], + "Nuclide": "Hg204", + "c [fm]": { + "value": 6.61, + "uncertainty": 0.0024 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + }, + "hahn_experimental_1979_fermi_Hg199": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2" + ], + "Nuclide": "Hg199", + "c [fm]": { + "value": 6.5741, + "uncertainty": 0.0027 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + }, + "hahn_experimental_1979_fermi_Hg201": { + "Reference": "hahn_experimental_1979", + "Relies On": [ + "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2" + ], + "Nuclide": "Hg201", + "c [fm]": { + "value": 6.5892, + "uncertainty": 0.0025 + }, + "a [fm]": { + "value": 0.5234, + "uncertainty": null + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "Fixed a, #NP_unc, #QED_unc, #Exp_unc" + } +} diff --git a/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy Difference (different nuclides).json new file mode 100644 index 0000000..21a0c95 --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,57 @@ +{ + "hahn_experimental_1979_muonic_difference_Hg198_Hg199_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide_A": "Hg198", + "Nuclide_B": "Hg199", + "Level": "1s1/2", + "Energy Difference [keV] (A-B)": { + "value": -1.48, + "uncertainty": 0.18 + }, + "Notes": "From 4f7/2-1s1/2" + }, + "hahn_experimental_1979_muonic_difference_Hg198_Hg200_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide_A": "Hg198", + "Nuclide_B": "Hg200", + "Level": "1s1/2", + "Energy Difference [keV] (A-B)": { + "value": -8.7, + "uncertainty": 0.15 + }, + "Notes": "From 4f7/2-1s1/2 shift" + }, + "hahn_experimental_1979_muonic_difference_Hg198_Hg201_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide_A": "Hg198", + "Nuclide_B": "Hg201", + "Level": "1s1/2", + "Energy Difference [keV] (A-B)": { + "value": -12.62, + "uncertainty": 0.27 + }, + "Notes": "From 4f7/2-1s1/2 shift" + }, + "hahn_experimental_1979_muonic_difference_Hg198_Hg202_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide_A": "Hg198", + "Nuclide_B": "Hg202", + "Level": "1s1/2", + "Energy Difference [keV] (A-B)": { + "value": 18.46, + "uncertainty": 0.1 + }, + "Notes": "From 4f7/2-1s1/2 shift" + }, + "hahn_experimental_1979_muonic_difference_Hg198_Hg204_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide_A": "Hg198", + "Nuclide_B": "Hg204", + "Level": "1s1/2", + "Energy Difference [keV] (A-B)": { + "value": -27.67, + "uncertainty": 0.15 + }, + "Notes": "From 4f7/2-1s1/2 shift" + } +} diff --git a/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy.json b/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy.json new file mode 100644 index 0000000..e1d4bd7 --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/Muonic Transition Energy.json @@ -0,0 +1,368 @@ +{ + "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 5839.37, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 5831.19, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 5824.08, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 5815.83, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 5665.89, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 5658.44, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 5649.95, + "Uncertainty": 0.52 + } + }, + "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 5642.36, + "Uncertainty": 0.54 + } + }, + "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 2398.98, + "Uncertainty": 0.17 + } + }, + "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 2398.16, + "Uncertainty": 0.17 + } + }, + "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 2395.49, + "Uncertainty": 0.16 + } + }, + "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 2394.15, + "Uncertainty": 0.19 + } + }, + "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 2533.28, + "Uncertainty": 0.2 + } + }, + "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 2532.62, + "Uncertainty": 0.2 + } + }, + "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 2530.34, + "Uncertainty": 0.19 + } + }, + "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 2528.83, + "Uncertainty": 0.22 + } + }, + "hahn_experimental_1979_muonic_Hg198_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 892.32, + "Uncertainty": 0.07 + } + }, + "hahn_experimental_1979_muonic_Hg200_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 892.51, + "Uncertainty": 0.07 + } + }, + "hahn_experimental_1979_muonic_Hg202_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 892.37, + "Uncertainty": 0.07 + } + }, + "hahn_experimental_1979_muonic_Hg204_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 892.43, + "Uncertainty": 0.07 + } + }, + "hahn_experimental_1979_muonic_Hg198_4f5/2_3d3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Hg198", + "Energy [keV]": { + "Value": 923.04, + "Uncertainty": 0.08 + } + }, + "hahn_experimental_1979_muonic_Hg200_4f5/2_3d3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Hg200", + "Energy [keV]": { + "Value": 923.1, + "Uncertainty": 0.08 + } + }, + "hahn_experimental_1979_muonic_Hg202_4f5/2_3d3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Hg202", + "Energy [keV]": { + "Value": 923.07, + "Uncertainty": 0.08 + } + }, + "hahn_experimental_1979_muonic_Hg204_4f5/2_3d3/2": { + "Reference": "hahn_experimental_1979", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Hg204", + "Energy [keV]": { + "Value": 922.99, + "Uncertainty": 0.08 + } + }, + "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg199", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 5660.63, + "uncertainty": 1.08 + }, + "Notes": "Corrected for dynamic effects" + }, + "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg199", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2529.55, + "uncertainty": 0.45 + }, + "Notes": "Corrected for dynamic effects" + }, + "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg199", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 892.46, + "uncertainty": 0.06 + }, + "Notes": "Corrected for dynamic effects" + }, + "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg201", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 5651.94, + "uncertainty": 0.9 + }, + "Notes": "Corrected for dynamic effects" + }, + "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg201", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 2528.57, + "uncertainty": 0.4 + }, + "Notes": "Corrected for dynamic effects" + }, + "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2": { + "Reference": "hahn_experimental_1979", + "Nuclide": "Hg201", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Energy [keV]": { + "value": 892.57, + "uncertainty": 0.1 + }, + "Notes": "Corrected for dynamic effects" + } +} diff --git a/radbase/compilation/hahn_experimental_1979/energies.txt b/radbase/compilation/hahn_experimental_1979/energies.txt new file mode 100644 index 0000000..3e72cb7 --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/energies.txt @@ -0,0 +1,7 @@ +, Hg198, Hg200, Hg202, Hg204 +2p3/2-1s1/2, 5839.37(12)(52),5831.19(11)(52),5824.08(08)(52),5815.83(13)(52) +2p1/2-1s1/2, 5665.89(16)(52),5658.44(16)(52),5649.95(14)(52),5642.36(20)(54) +3d5/2-2p3/2, 2398.98(10)(17),2398.16(10)(17),2395.49(08)(16),2394.15(12)(19) +3d3/2-2p1/2, 2533.28(14)(20),2532.62(14)(20),2530.34(12)(19),2528.83(17)(22) +4f7/2-3d5/2, 892.32(04)(07),892.51(04)(07),892.37(04)(07),892.43(04)(07) +4f5/2-3d3/2, 923.04(04)(08),923.10(05)(08),923.07(05)(08),922.99(05)(08) diff --git a/radbase/compilation/hahn_experimental_1979/hahn_1979_process.py b/radbase/compilation/hahn_experimental_1979/hahn_1979_process.py new file mode 100644 index 0000000..3000c77 --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/hahn_1979_process.py @@ -0,0 +1,32 @@ +import csv + +from uncertainties import ufloat_fromstr + +from radbase.data_entry import (DataEntryInterface, + muonic_transition_energy_template) + +values: dict = { + 'Reference': 'hahn_experimental_1979' +} + +interface = DataEntryInterface(start_interface=False) + +with open('./energies.txt', 'r') as f: + reader = list(csv.reader(f, delimiter=',')) + + elements = reader[0][1:] + for row in reader[1:]: + transition, energies = row[0].strip(), row[1:] + + transition = {side: level for side, level in zip(['Upper', 'Lower'], transition.split('-'))} + values['Transition'] = transition + + for nuclide, energy in zip(elements, energies): + nuclide, energy = nuclide.strip(), energy.strip() + values['Nuclide'] = nuclide + first_par, last_par = energy.find('('), energy.find(')') + energy = ufloat_fromstr(energy[:first_par] + energy[last_par + 1:]) + values['Energy [keV]'] = {'Value': energy.n, + 'Uncertainty': energy.s} + + interface.save_data(muonic_transition_energy_template, values, replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/hahn_experimental_1979/notes.txt b/radbase/compilation/hahn_experimental_1979/notes.txt new file mode 100644 index 0000000..a79b2ea --- /dev/null +++ b/radbase/compilation/hahn_experimental_1979/notes.txt @@ -0,0 +1,4 @@ +Measured muonic transition energies up to 4f7/2 for Hg 198, 199, 200, 201, 202, and 204. Much of the paper is focused on +extracting quadrapole moments, but a two parameter Fermi fit is performed as well. This fit includes the 2p->1s, 3d->2p +and 2p FS splitting. Isotope shifts are presented as a shift in the 1s1/2 level by looking at the 4f7/2->1s1/2 isotope +shifts. These shifts are then converted into shifts in Barrett radii using alpha from Engfer 74. diff --git a/radbase/compilation/kast_isotone_1971/Fermi Distribution.json b/radbase/compilation/kast_isotone_1971/Fermi Distribution.json new file mode 100644 index 0000000..21b9439 --- /dev/null +++ b/radbase/compilation/kast_isotone_1971/Fermi Distribution.json @@ -0,0 +1,208 @@ +{ + "kast_isotone_1971_fermi_Cd114": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2" + ], + "Nuclide": "Cd114", + "c [fm]": { + "value": 5.27, + "uncertainty": 0.11 + }, + "a [fm]": { + "value": 0.58, + "uncertainty": 0.05 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + }, + "kast_isotone_1971_fermi_In115": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2" + ], + "Nuclide": "In115", + "c [fm]": { + "value": 5.38, + "uncertainty": 0.19 + }, + "a [fm]": { + "value": 0.53, + "uncertainty": 0.1 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + }, + "kast_isotone_1971_fermi_Sn116": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2" + ], + "Nuclide": "Sn116", + "c [fm]": { + "value": 5.26, + "uncertainty": 0.08 + }, + "a [fm]": { + "value": 0.6, + "uncertainty": 0.03 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + }, + "kast_isotone_1971_fermi_Sn124": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2" + ], + "Nuclide": "Sn124", + "c [fm]": { + "value": 5.3, + "uncertainty": 0.07 + }, + "a [fm]": { + "value": 0.61, + "uncertainty": 0.03 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + }, + "kast_isotone_1971_fermi_Te126": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2" + ], + "Nuclide": "Te126", + "c [fm]": { + "value": 5.43, + "uncertainty": 0.07 + }, + "a [fm]": { + "value": 0.59, + "uncertainty": 0.03 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + }, + "kast_isotone_1971_fermi_I127": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2" + ], + "Nuclide": "I127", + "c [fm]": { + "value": 5.51, + "uncertainty": 0.06 + }, + "a [fm]": { + "value": 2.49, + "uncertainty": 0.08 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/kast_isotone_1971/Muonic Radius.json b/radbase/compilation/kast_isotone_1971/Muonic Radius.json new file mode 100644 index 0000000..de4c8f3 --- /dev/null +++ b/radbase/compilation/kast_isotone_1971/Muonic Radius.json @@ -0,0 +1,92 @@ +{ + "kast_isotone_1971_radius_Cd114_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_Cd114" + ], + "Nuclide": "Cd114", + "R [fm]": { + "value": 4.624, + "uncertainty": 0.008 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "kast_isotone_1971_radius_In115_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_In115" + ], + "Nuclide": "In115", + "R [fm]": { + "value": 4.619, + "uncertainty": 0.015 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "kast_isotone_1971_radius_Sn116_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_Sn116" + ], + "Nuclide": "Sn116", + "R [fm]": { + "value": 4.642, + "uncertainty": 0.006 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "kast_isotone_1971_radius_Sn124_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_Sn124" + ], + "Nuclide": "Sn124", + "R [fm]": { + "value": 4.698, + "uncertainty": 0.006 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "kast_isotone_1971_radius_Te126_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_Te126" + ], + "Nuclide": "Te126", + "R [fm]": { + "value": 4.774, + "uncertainty": 0.006 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + }, + "kast_isotone_1971_radius_I127_NP_Calculated": { + "Reference": "kast_isotone_1971", + "Relies On": [ + "kast_isotone_1971_fermi_I127" + ], + "Nuclide": "I127", + "R [fm]": { + "value": 4.763, + "uncertainty": 0.006 + }, + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Reduced Chi-Squared": 0.0, + "Notes": "" + } +} diff --git a/radbase/compilation/kast_isotone_1971/Muonic Transition Energy.json b/radbase/compilation/kast_isotone_1971/Muonic Transition Energy.json new file mode 100644 index 0000000..f0bb6b0 --- /dev/null +++ b/radbase/compilation/kast_isotone_1971/Muonic Transition Energy.json @@ -0,0 +1,314 @@ +{ + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Cd114", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3263.63, + "uncertainty": 0.37 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Cd114", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3223.74, + "uncertainty": 0.46 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Cd114", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 905.85, + "uncertainty": 0.26 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Cd114", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 940.58, + "uncertainty": 0.23 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "In115", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3366.27, + "uncertainty": 0.42 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "In115", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3322.67, + "uncertainty": 0.42 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "In115", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 982.23, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "In115", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 981.64, + "uncertainty": 0.48 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn116", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3464.78, + "uncertainty": 0.47 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn116", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3419.06, + "uncertainty": 0.4 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn116", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 982.23, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn116", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1022.09, + "uncertainty": 0.23 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn124", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3444.29, + "uncertainty": 0.35 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn124", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3398.91, + "uncertainty": 0.36 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn124", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 981.69, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Sn124", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1021.42, + "uncertainty": 0.21 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Te126", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3629.26, + "uncertainty": 0.42 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Te126", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3577.63, + "uncertainty": 0.58 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Te126", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1060.66, + "uncertainty": 0.22 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "Te126", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1105.66, + "uncertainty": 0.23 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_I127_2p3/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "I127", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3723.23, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_I127_2p1/2_1s1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "I127", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Energy [keV]": { + "value": 3667.35, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_I127_3d5/2_2p3/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "I127", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Energy [keV]": { + "value": 1101.84, + "uncertainty": 0.2 + }, + "Notes": "" + }, + "kast_isotone_1971_muonic_I127_3d3/2_2p1/2": { + "Reference": "kast_isotone_1971", + "Nuclide": "I127", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Energy [keV]": { + "value": 1150.42, + "uncertainty": 0.15 + }, + "Notes": "" + } +} diff --git a/radbase/compilation/phan_nuclear_1985/Calculated Muonic Nuclear Polarization.json b/radbase/compilation/phan_nuclear_1985/Calculated Muonic Nuclear Polarization.json new file mode 100644 index 0000000..3bde1ff --- /dev/null +++ b/radbase/compilation/phan_nuclear_1985/Calculated Muonic Nuclear Polarization.json @@ -0,0 +1,12 @@ +{ + "phan_nuclear_1985_muonic_nuclear_polarization_Zr90_1s1/2": { + "Reference": "phan_nuclear_1985", + "Nuclide": "Zr90", + "Level": "1s1/2", + "Energy [keV]": { + "value": 1067.0, + "uncertainty": null + }, + "Notes": "" + } +} diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json index 298cf7e..4c21e58 100644 --- a/radbase/compilation/references.json +++ b/radbase/compilation/references.json @@ -172,5 +172,94 @@ "pages": "609-619", "url": "https://link.aps.org/doi/10.1103/PhysRevC.32.609", "doi": "10.1103/PhysRevC.32.609" + }, + "kast_isotone_1971": { + "title": "THE ISOTONE SHIFT IN MUONIC X-RAYS IN THE TIN REGION", + "author": [ + "J. W. KAST", + "S. BERNOW", + "S. C. CHENG", + "D. HLTLIN", + "W. Y. LEE", + "E. R. MACAGNO", + "A. M. RUSHTON", + "C. S. WU" + ], + "year": "1971", + "month": "June", + "journal": "Nuclear Physics A", + "volume": "169", + "pages": "62-70", + "url": "https://linkinghub.elsevier.com/retrieve/pii/0375947471905586", + "doi": "10.1016/0375-9474(71)90558-6" + }, + "hahn_experimental_1979": { + "title": "An experimental study of muonic X-ray transitions in mercury isotopes", + "author": [ + "A. A. Hahn", + "J. P. Miller", + "R. J. Powers", + "A. Zehnder", + "A. M. Rushton", + "R. E. Welsh", + "A. R. Kunselman", + "P. Roberson", + "H. K. Walter" + ], + "year": "1979", + "month": "February", + "journal": "Nuclear Physics A", + "volume": "314", + "pages": "361-386", + "url": "https://www.sciencedirect.com/science/article/pii/0375947479906043", + "doi": "10.1016/0375-9474(79)90604-3" + }, + "saito_muonic_2025": { + "title": "Muonic x-ray measurement for the nuclear charge distribution: The case of stable palladium isotopes", + "author": [ + "T. Y. Saito", + "M. Niikura", + "T. Matsuzaki", + "H. Sakurai", + "M. Igashira", + "H. Imao", + "K. Ishida", + "T. Katabuchi", + "Y. Kawashima", + "M. K. Kubo", + "Y. Miyake", + "Y. Mori", + "K. Ninomiya", + "A. Sato", + "K. Shimomura", + "P. Strasser", + "A. Taniguchi", + "D. Tomono", + "Y. Watanabe" + ], + "year": "2025", + "month": "March", + "journal": "Physical Review C", + "volume": "Volume 111", + "pages": "034313", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.111.034313", + "doi": "10.1103/PhysRevC.111.034313" + }, + "wolfhahrt_nuclear_1981": { + "title": "Nuclear charge distributions in 1f7\\2-shell nuclei from muonic x-ray measurements", + "author": [ + "H. D. Wolfhahrt", + "E. B. Shera", + "M. V. Hoehn", + "Y. Yamazaki", + "R. M. Steffen" + ], + "year": "1981", + "month": "January", + "journal": "Physical Review C", + "volume": "23", + "pages": "533-548", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.23.533", + "doi": "10.1103/PhysRevC.23.533" } } diff --git a/radbase/compilation/saito_muonic_2025/Fermi Distribution.json b/radbase/compilation/saito_muonic_2025/Fermi Distribution.json new file mode 100644 index 0000000..a594e33 --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/Fermi Distribution.json @@ -0,0 +1,110 @@ +{ + "saito_muonic_2025_fermi_Pd104": { + "Reference": "saito_muonic_2025", + "Relies On": [ + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2" + ], + "Nuclide": "Pd104", + "c [fm]": { + "value": 5.26, + "uncertainty": 0.12 + }, + "a [fm]": { + "value": 2.25, + "uncertainty": 0.25 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "No theoretical uncertainties. #Exp_unc" + }, + "saito_muonic_2025_fermi_Pd106": { + "Reference": "saito_muonic_2025", + "Relies On": [ + "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2" + ], + "Nuclide": "Pd106", + "c [fm]": { + "value": 5.49, + "uncertainty": 0.3 + }, + "a [fm]": { + "value": 1.76, + "uncertainty": 0.65 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "No theoretical uncertainties. #Exp_unc" + }, + "saito_muonic_2025_fermi_Pd108": { + "Reference": "saito_muonic_2025", + "Relies On": [ + "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2" + ], + "Nuclide": "Pd108", + "c [fm]": { + "value": 5.45, + "uncertainty": 0.11 + }, + "a [fm]": { + "value": 1.96, + "uncertainty": 0.27 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "No theoretical uncertainties. #Exp_unc" + }, + "saito_muonic_2025_fermi_Pd110": { + "Reference": "saito_muonic_2025", + "Relies On": [ + "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2" + ], + "Nuclide": "Pd110", + "c [fm]": { + "value": 5.6, + "uncertainty": 0.26 + }, + "a [fm]": { + "value": 1.61, + "uncertainty": 0.7 + }, + "beta2 [-]": { + "value": 0.0, + "uncertainty": null + }, + "beta4 [-]": { + "value": 0.0, + "uncertainty": null + }, + "Notes": "No theoretical uncertainties. #Exp_unc" + } +} diff --git a/radbase/compilation/saito_muonic_2025/Muonic Barrett Moment.json b/radbase/compilation/saito_muonic_2025/Muonic Barrett Moment.json new file mode 100644 index 0000000..cefdb02 --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/Muonic Barrett Moment.json @@ -0,0 +1,467 @@ +{ + "saito_muonic_2025_barrett_moment_Pb104_2p1/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2" + ], + "Nuclide": "Pb104", + "Rka [fm]": { + "value": 5.762, + "uncertainty": 0.002 + }, + "k [-]": "2.163", + "alpha [1/fm]": "0.1037", + "Cz [fm/keV]": "0", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc" + }, + "saito_muonic_2025_barrett_moment_Pd104_2p1/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2" + ], + "alpha [1/fm]": "0.1037", + "k [-]": "2.163", + "Rka [fm]": { + "Value": 5.762, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_2p3/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2" + ], + "alpha [1/fm]": "0.1013", + "k [-]": "2.145", + "Rka [fm]": { + "Value": 5.764, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_3d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0802", + "k [-]": "3.705", + "Rka [fm]": { + "Value": 5.91, + "Uncertainty": 0.02 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_3d3/2-2p1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2" + ], + "alpha [1/fm]": "0.1183", + "k [-]": "3.798", + "Rka [fm]": { + "Value": 5.89, + "Uncertainty": 0.04 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_4d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0795", + "k [-]": "3.703", + "Rka [fm]": { + "Value": 5.9, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_4f7/2-3d5/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2" + ], + "alpha [1/fm]": "0.1257", + "k [-]": "5.864", + "Rka [fm]": { + "Value": 6.1, + "Uncertainty": 0.4 + } + }, + "saito_muonic_2025_barrett_moment_Pd104_4f5/2-3d3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd104", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2" + ], + "alpha [1/fm]": "0.0963", + "k [-]": "6.252", + "Rka [fm]": { + "Value": 6.3, + "Uncertainty": 0.6 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_2p1/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2" + ], + "alpha [1/fm]": "0.1027", + "k [-]": "2.157", + "Rka [fm]": { + "Value": 5.792, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_2p3/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2" + ], + "alpha [1/fm]": "0.1013", + "k [-]": "2.148", + "Rka [fm]": { + "Value": 5.795, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_3d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0802", + "k [-]": "3.705", + "Rka [fm]": { + "Value": 5.92, + "Uncertainty": 0.07 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_3d3/2-2p1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2" + ], + "alpha [1/fm]": "0.1184", + "k [-]": "3.798", + "Rka [fm]": { + "Value": 5.86, + "Uncertainty": 0.04 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_4d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0795", + "k [-]": "3.703", + "Rka [fm]": { + "Value": 5.77, + "Uncertainty": 0.09 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_4f7/2-3d5/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2" + ], + "alpha [1/fm]": "0.1257", + "k [-]": "5.864", + "Rka [fm]": { + "Value": 5.6, + "Uncertainty": 0.7 + } + }, + "saito_muonic_2025_barrett_moment_Pd106_4f5/2-3d3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd106", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2" + ], + "alpha [1/fm]": "0.0963", + "k [-]": "6.251", + "Rka [fm]": { + "Value": 5.6, + "Uncertainty": 0.8 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_2p1/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2" + ], + "alpha [1/fm]": "0.1020", + "k [-]": "2.153", + "Rka [fm]": { + "Value": 5.822, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_2p3/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2" + ], + "alpha [1/fm]": "0.1012", + "k [-]": "2.149", + "Rka [fm]": { + "Value": 5.824, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_3d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0799", + "k [-]": "3.705", + "Rka [fm]": { + "Value": 5.95, + "Uncertainty": 0.02 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_3d3/2-2p1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2" + ], + "alpha [1/fm]": "0.1184", + "k [-]": "3.798", + "Rka [fm]": { + "Value": 5.91, + "Uncertainty": 0.01 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_4d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0793", + "k [-]": "3.702", + "Rka [fm]": { + "Value": 5.87, + "Uncertainty": 0.07 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_4f7/2-3d5/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2" + ], + "alpha [1/fm]": "0.1257", + "k [-]": "5.864", + "Rka [fm]": { + "Value": 5.8, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_barrett_moment_Pd108_4f5/2-3d3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd108", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2" + ], + "alpha [1/fm]": "0.0963", + "k [-]": "6.252", + "Rka [fm]": { + "Value": 6.3, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_2p1/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2" + ], + "alpha [1/fm]": "0.1013", + "k [-]": "2.149", + "Rka [fm]": { + "Value": 5.849, + "Uncertainty": 0.003 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_2p3/2-1s1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2" + ], + "alpha [1/fm]": "0.1013", + "k [-]": "2.153", + "Rka [fm]": { + "Value": 5.856, + "Uncertainty": 0.002 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_3d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0799", + "k [-]": "3.704", + "Rka [fm]": { + "Value": 5.94, + "Uncertainty": 0.05 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_3d3/2-2p1/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2" + ], + "alpha [1/fm]": "0.1184", + "k [-]": "3.798", + "Rka [fm]": { + "Value": 5.92, + "Uncertainty": 0.04 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_4d5/2-2p3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2" + ], + "alpha [1/fm]": "0.0793", + "k [-]": "3.702", + "Rka [fm]": { + "Value": 5.9, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_4f7/2-3d5/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2" + ], + "alpha [1/fm]": "0.1257", + "k [-]": "5.864", + "Rka [fm]": { + "Value": 6.1, + "Uncertainty": 0.4 + } + }, + "saito_muonic_2025_barrett_moment_Pd110_4f5/2-3d3/2": { + "Reference": "saito_muonic_2025", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "No theoretical uncertainties. #Exp_unc", + "Nuclide": "Pd110", + "Previous Muonic Measurements": [ + "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2" + ], + "alpha [1/fm]": "0.0963", + "k [-]": "6.252", + "Rka [fm]": { + "Value": 6.3, + "Uncertainty": 0.8 + } + } +} diff --git a/radbase/compilation/saito_muonic_2025/Muonic Transition Energy.json b/radbase/compilation/saito_muonic_2025/Muonic Transition Energy.json new file mode 100644 index 0000000..e312698 --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/Muonic Transition Energy.json @@ -0,0 +1,338 @@ +{ + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 3057.8, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 3091.7, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 833.4, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 863.6, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 1122.5, + "Uncertainty": 0.6 + } + }, + "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 291.6, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Pd104", + "Energy [keV]": { + "Value": 294.9, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 3050.3, + "Uncertainty": 0.5 + } + }, + "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 3084.0, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 833.4, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 863.8, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 1124.8, + "Uncertainty": 0.4 + } + }, + "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 291.7, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Pd106", + "Energy [keV]": { + "Value": 295.1, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 3042.9, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 3076.6, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 833.3, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 863.5, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 1124.4, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 291.6, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Pd108", + "Energy [keV]": { + "Value": 294.9, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p1/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 3036.2, + "Uncertainty": 0.7 + } + }, + "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 3068.8, + "Uncertainty": 0.4 + } + }, + "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 833.4, + "Uncertainty": 0.2 + } + }, + "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "3d3/2", + "Lower": "2p1/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 863.4, + "Uncertainty": 0.3 + } + }, + "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4d5/2", + "Lower": "2p3/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 1124.2, + "Uncertainty": 0.5 + } + }, + "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f7/2", + "Lower": "3d5/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 291.6, + "Uncertainty": 0.1 + } + }, + "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2": { + "Reference": "saito_muonic_2025", + "Transition": { + "Upper": "4f5/2", + "Lower": "3d3/2" + }, + "Nuclide": "Pd110", + "Energy [keV]": { + "Value": 294.9, + "Uncertainty": 0.2 + } + } +} diff --git a/radbase/compilation/saito_muonic_2025/notes.txt b/radbase/compilation/saito_muonic_2025/notes.txt new file mode 100644 index 0000000..5762127 --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/notes.txt @@ -0,0 +1,4 @@ +Measured muonic transition energies for 1s - 4f7/2 levels with >0.1 keV uncertainty for Pd104, 105, 106, 108, 110 and +fit 2pF distribution for all even isotopes using the 1s-2p and 2p-3d transition energies. Radii do not include any +theoretical uncertainties, and the confidence bands are assymetric. The lower bands are often much stricter than the +upper bands. Barrett radii are also provided, with uncertainty from theory only. diff --git a/radbase/compilation/saito_muonic_2025/saito_2025_process.py b/radbase/compilation/saito_muonic_2025/saito_2025_process.py new file mode 100644 index 0000000..d616e5b --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/saito_2025_process.py @@ -0,0 +1,49 @@ +import csv + +from uncertainties import ufloat_fromstr + +from radbase.data_entry import (DataEntryInterface, + muonic_barret_theory_template, + muonic_transition_energy_template) + +evalues: dict = { + 'Reference': 'saito_muonic_2025' +} + +bvalues: dict = { + 'Reference': 'saito_muonic_2025', + 'Nuclear Polarization Method': 'Calculated', + 'Calculated Nuclear Polarization': [], + 'Notes': 'No theoretical uncertainties. #Exp_unc' +} + +interface = DataEntryInterface(start_interface=False) + +with open('./values.txt', 'r') as f: + reader = list(csv.reader(f, delimiter=',')) + + for row in reader: + nuclide, transition, energy, k, alpha, rka = row + + nuclide = nuclide[3:] + nuclide[:-2] + + transition = {side: level for side, level in zip(['Upper', 'Lower'], transition.split('-'))} + evalues['Transition'] = transition + + nuclide, energy = nuclide.strip(), energy.strip() + evalues['Nuclide'], bvalues['Nuclide'] = nuclide, nuclide + + energy = ufloat_fromstr(energy) + evalues['Energy [keV]'] = {'Value': energy.n, + 'Uncertainty': energy.s} + + interface.save_data(muonic_transition_energy_template, evalues, replacement_strategy='AlwaysReplace') + + bvalues['Previous Muonic Measurements'] = [muonic_transition_energy_template.data_key(evalues)] + bvalues['alpha [1/fm]'] = alpha + bvalues["k [-]"] = k + rka = ufloat_fromstr(rka) + bvalues['Rka [fm]'] = {'Value': rka.n, + 'Uncertainty': rka.s} + + interface.save_data(muonic_barret_theory_template, bvalues, replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/saito_muonic_2025/values.txt b/radbase/compilation/saito_muonic_2025/values.txt new file mode 100644 index 0000000..a2794fe --- /dev/null +++ b/radbase/compilation/saito_muonic_2025/values.txt @@ -0,0 +1,28 @@ +104Pd,2p1/2-1s1/2,3057.8(3),2.163,0.1037,5.762(2) +104Pd,2p3/2-1s1/2,3091.7(2),2.145,0.1013,5.764(2) +104Pd,3d5/2-2p3/2,833.4(1),3.705,0.0802,5.91(2) +104Pd,3d3/2-2p1/2,863.6(3),3.798,0.1183,5.89(4) +104Pd,4d5/2-2p3/2,1122.5(6),3.703,0.0795,5.9(1) +104Pd,4f7/2-3d5/2,291.6(1),5.864,0.1257,6.1(4) +104Pd,4f5/2-3d3/2,294.9(2),6.252,0.0963,6.3(6) +106Pd,2p1/2-1s1/2,3050.3(5),2.157,0.1027,5.792(2) +106Pd,2p3/2-1s1/2,3084.0(3),2.148,0.1013,5.795(2) +106Pd,3d5/2-2p3/2,833.4(3),3.705,0.0802,5.92(7) +106Pd,3d3/2-2p1/2,863.8(3),3.798,0.1184,5.86(4) +106Pd,4d5/2-2p3/2,1124.8(4),3.703,0.0795,5.77(9) +106Pd,4f7/2-3d5/2,291.7(2),5.864,0.1257,5.6(7) +106Pd,4f5/2-3d3/2,295.1(3),6.251,0.0963,5.6(8) +108Pd,2p1/2-1s1/2,3042.9(2),2.153,0.1020,5.822(2) +108Pd,2p3/2-1s1/2,3076.6(2),2.149,0.1012,5.824(2) +108Pd,3d5/2-2p3/2,833.3(1),3.705,0.0799,5.95(2) +108Pd,3d3/2-2p1/2,863.5(1),3.798,0.1184,5.91(1) +108Pd,4d5/2-2p3/2,1124.4(3),3.702,0.0793,5.87(7) +108Pd,4f7/2-3d5/2,291.6(1),5.864,0.1257,5.8(3) +108Pd,4f5/2-3d3/2,294.9(1),6.252,0.0963,6.3(3) +110Pd,2p1/2-1s1/2,3036.2(7),2.149,0.1013,5.849(3) +110Pd,2p3/2-1s1/2,3068.8(4),2.153,0.1013,5.856(2) +110Pd,3d5/2-2p3/2,833.4(2),3.704,0.0799,5.94(5) +110Pd,3d3/2-2p1/2,863.4(3),3.798,0.1184,5.92(4) +110Pd,4d5/2-2p3/2,1124.2(5),3.702,0.0793,5.9(1) +110Pd,4f7/2-3d5/2,291.6(1),5.864,0.1257,6.1(4) +110Pd,4f5/2-3d3/2,294.9(2),6.252,0.0963,6.3(8) diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json new file mode 100644 index 0000000..aa8cc27 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,2956 @@ +{ + "wolfhahrt_nuclear_1981_muonic_difference_wRo_lumnCo_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "wRo", + "Nuclide_B": "lumnCo", + "Energy Difference [keV] (A-B)": { + "Value": "Value", + "Uncertainty": "Uncertainty" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_K41_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "K41", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "-0.349", + "Uncertainty": "0.024" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca40", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "71.062", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca40", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "71.411", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca42", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "70.251", + "Uncertainty": "0.043" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca42", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "70.600", + "Uncertainty": "0.040" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca42", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "-0.811", + "Uncertainty": "0.016" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca43", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "70.693", + "Uncertainty": "0.042" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca43", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "71.042", + "Uncertainty": "0.039" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca43", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "-0.369", + "Uncertainty": "0.015" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca43", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "0.442", + "Uncertainty": "0.016" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca44", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "70.038", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca44", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "70.387", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca44", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "-1.024", + "Uncertainty": "0.013" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca44", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "-0.213", + "Uncertainty": "0.016" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca44", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "-0.655", + "Uncertainty": "0.014" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "70.699", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "71.048", + "Uncertainty": "0.111" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "-0.363", + "Uncertainty": "0.105" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "0.448", + "Uncertainty": "0.106" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "0.006", + "Uncertainty": "0.106" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca46", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "0.661", + "Uncertainty": "0.106" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "71.369", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "71.718", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "0.307", + "Uncertainty": "0.012" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "1.118", + "Uncertainty": "0.015" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "0.676", + "Uncertainty": "0.016" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "1.331", + "Uncertainty": "0.014" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ca48", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "0.670", + "Uncertainty": "0.106" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "143.877", + "Uncertainty": "0.043" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "144.226", + "Uncertainty": "0.040" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "72.815", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "73.626", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "73.184", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "73.839", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "73.178", + "Uncertainty": "0.109" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Sc45", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "72.508", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "218.876", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "219.225", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "147.814", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "148.625", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "148.183", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "148.838", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "148.177", + "Uncertainty": "0.108" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "147.507", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti46", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "74.999", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "219.356", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "219.705", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "148.294", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "149.105", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "148.663", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "149.318", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "148.657", + "Uncertainty": "0.108" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "147.987", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "75.479", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti47", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "0.480", + "Uncertainty": "0.019" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "219.534", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "219.883", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "148.472", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "149.283", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "148.841", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "149.496", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "148.835", + "Uncertainty": "0.109" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "148.165", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "75.657", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "0.658", + "Uncertainty": "0.023" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "0.178", + "Uncertainty": "0.019" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "220.308", + "Uncertainty": "0.046" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "220.657", + "Uncertainty": "0.043" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "149.246", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "150.057", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "149.615", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "150.270", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "149.609", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "148.939", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "76.431", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "1.432", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "0.952", + "Uncertainty": "0.025" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti49", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "0.774", + "Uncertainty": "0.027" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "220.470", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "220.819", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "149.408", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "150.219", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "149.777", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "150.432", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "149.771", + "Uncertainty": "0.109" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "149.101", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "76.593", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "1.594", + "Uncertainty": "0.023" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "1.114", + "Uncertainty": "0.022" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "0.936", + "Uncertainty": "0.022" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "299.083", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "299.432", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "228.021", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "228.832", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "228.390", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "229.045", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "228.384", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "227.714", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "155.206", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "80.207", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "79.727", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "79.549", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "378.060", + "Uncertainty": "0.042" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "378.409", + "Uncertainty": "0.039" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "306.998", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "307.809", + "Uncertainty": "0.039" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "307.367", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "308.022", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "307.361", + "Uncertainty": "0.111" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "306.691", + "Uncertainty": "0.039" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "234.183", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "159.184", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "158.704", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "158.526", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "379.168", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "379.517", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "308.106", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "308.917", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "308.475", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "309.130", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "308.469", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "307.799", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "235.291", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "160.292", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "159.812", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "159.634", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "378.263", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "378.612", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "307.201", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "308.012", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "307.570", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "308.225", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "307.564", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "306.894", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "234.386", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "159.387", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "158.907", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "158.729", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "376.770", + "Uncertainty": "0.045" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "377.119", + "Uncertainty": "0.042" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "305.708", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "306.519", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "306.077", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "306.732", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "306.071", + "Uncertainty": "0.111" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "305.401", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "232.893", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "157.894", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "157.414", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "157.236", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "459.736", + "Uncertainty": "0.046" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "460.085", + "Uncertainty": "0.045" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "388.674", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "389.485", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "389.043", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "389.698", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "389.037", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "388.367", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "315.859", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "240.860", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "240.380", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "240.202", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "K39", + "Energy Difference [keV] (A-B)": { + "Value": "543.924", + "Uncertainty": "0.041" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "K41", + "Energy Difference [keV] (A-B)": { + "Value": "544.273", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca40", + "Energy Difference [keV] (A-B)": { + "Value": "472.862", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca42", + "Energy Difference [keV] (A-B)": { + "Value": "473.673", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca43", + "Energy Difference [keV] (A-B)": { + "Value": "473.231", + "Uncertainty": "0.037" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca44", + "Energy Difference [keV] (A-B)": { + "Value": "473.886", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca46", + "Energy Difference [keV] (A-B)": { + "Value": "473.225", + "Uncertainty": "0.110" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ca48", + "Energy Difference [keV] (A-B)": { + "Value": "472.555", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Sc45", + "Energy Difference [keV] (A-B)": { + "Value": "400.047", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ti46", + "Energy Difference [keV] (A-B)": { + "Value": "325.048", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ti47", + "Energy Difference [keV] (A-B)": { + "Value": "324.568", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ti48", + "Energy Difference [keV] (A-B)": { + "Value": "324.390", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Mn55_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Mn55", + "Energy Difference [keV] (A-B)": { + "Value": "84.188", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr54_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Cr54", + "Energy Difference [keV] (A-B)": { + "Value": "167.154", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Cr53", + "Energy Difference [keV] (A-B)": { + "Value": "165.661", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Cr52", + "Energy Difference [keV] (A-B)": { + "Value": "164.756", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Cr50", + "Energy Difference [keV] (A-B)": { + "Value": "165.864", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "244.841", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "323.454", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Fe56", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "323.616", + "Uncertainty": "0.038" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr54_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Cr54", + "Energy Difference [keV] (A-B)": { + "Value": "82.966", + "Uncertainty": "0.028" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Cr53", + "Energy Difference [keV] (A-B)": { + "Value": "81.473", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Cr52", + "Energy Difference [keV] (A-B)": { + "Value": "80.568", + "Uncertainty": "0.029" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Cr50", + "Energy Difference [keV] (A-B)": { + "Value": "81.676", + "Uncertainty": "0.033" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "160.653", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "239.266", + "Uncertainty": "0.032" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Mn55", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "239.428", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr53", + "Energy Difference [keV] (A-B)": { + "Value": "-1.493", + "Uncertainty": "0.022" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Energy Difference [keV] (A-B)": { + "Value": "-2.398", + "Uncertainty": "0.020" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Energy Difference [keV] (A-B)": { + "Value": "-1.290", + "Uncertainty": "0.027" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "77.687", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "156.300", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr54", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "156.462", + "Uncertainty": "0.035" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Cr52", + "Energy Difference [keV] (A-B)": { + "Value": "-0.905", + "Uncertainty": "0.019" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Cr50", + "Energy Difference [keV] (A-B)": { + "Value": "0.203", + "Uncertainty": "0.028" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "79.180", + "Uncertainty": "0.026" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "157.793", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr53", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "157.955", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Energy Difference [keV] (A-B)": { + "Value": "1.108", + "Uncertainty": "0.022" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "80.085", + "Uncertainty": "0.024" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "158.698", + "Uncertainty": "0.027" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr52", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "158.860", + "Uncertainty": "0.030" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "V51", + "Energy Difference [keV] (A-B)": { + "Value": "78.977", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "157.590", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Cr50", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "157.752", + "Uncertainty": "0.036" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ti50", + "Energy Difference [keV] (A-B)": { + "Value": "78.613", + "Uncertainty": "0.031" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "V51", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "78.775", + "Uncertainty": "0.034" + } + }, + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide_A": "Ti50", + "Nuclide_B": "Ti49", + "Energy Difference [keV] (A-B)": { + "Value": "0.162", + "Uncertainty": "0.027" + } + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv b/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv new file mode 100644 index 0000000..5056334 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv @@ -0,0 +1,211 @@ +Row,Column,Value,Uncertainty +41K,39K,-0.349,0.024 +40Ca,39K,71.062,0.041 +40Ca,41K,71.411,0.038 +42Ca,39K,70.251,0.043 +42Ca,41K,70.600,0.040 +42Ca,40Ca,-0.811,0.016 +43Ca,39K,70.693,0.042 +43Ca,41K,71.042,0.039 +43Ca,40Ca,-0.369,0.015 +43Ca,42Ca,0.442,0.016 +44Ca,39K,70.038,0.041 +44Ca,41K,70.387,0.038 +44Ca,40Ca,-1.024,0.013 +44Ca,42Ca,-0.213,0.016 +44Ca,43Ca,-0.655,0.014 +46Ca,39K,70.699,0.110 +46Ca,41K,71.048,0.111 +46Ca,40Ca,-0.363,0.105 +46Ca,42Ca,0.448,0.106 +46Ca,43Ca,0.006,0.106 +46Ca,44Ca,0.661,0.106 +48Ca,39K,71.369,0.041 +48Ca,41K,71.718,0.038 +48Ca,40Ca,0.307,0.012 +48Ca,42Ca,1.118,0.015 +48Ca,43Ca,0.676,0.016 +48Ca,44Ca,1.331,0.014 +48Ca,46Ca,0.670,0.106 +45Sc,39K,143.877,0.043 +45Sc,41K,144.226,0.040 +45Sc,40Ca,72.815,0.032 +45Sc,42Ca,73.626,0.034 +45Sc,43Ca,73.184,0.033 +45Sc,44Ca,73.839,0.032 +45Sc,46Ca,73.178,0.109 +45Sc,48Ca,72.508,0.033 +46Ti,39K,218.876,0.041 +46Ti,41K,219.225,0.038 +46Ti,40Ca,147.814,0.029 +46Ti,42Ca,148.625,0.032 +46Ti,43Ca,148.183,0.031 +46Ti,44Ca,148.838,0.030 +46Ti,46Ca,148.177,0.108 +46Ti,48Ca,147.507,0.030 +46Ti,45Sc,74.999,0.029 +47Ti,39K,219.356,0.041 +47Ti,41K,219.705,0.038 +47Ti,40Ca,148.294,0.029 +47Ti,42Ca,149.105,0.032 +47Ti,43Ca,148.663,0.031 +47Ti,44Ca,149.318,0.030 +47Ti,46Ca,148.657,0.108 +47Ti,48Ca,147.987,0.031 +47Ti,45Sc,75.479,0.029 +47Ti,46Ti,0.480,0.019 +48Ti,39K,219.534,0.041 +48Ti,41K,219.883,0.038 +48Ti,40Ca,148.472,0.032 +48Ti,42Ca,149.283,0.033 +48Ti,43Ca,148.841,0.031 +48Ti,44Ca,149.496,0.032 +48Ti,46Ca,148.835,0.109 +48Ti,48Ca,148.165,0.033 +48Ti,45Sc,75.657,0.032 +48Ti,46Ti,0.658,0.023 +48Ti,47Ti,0.178,0.019 +49Ti,39K,220.308,0.046 +49Ti,41K,220.657,0.043 +49Ti,40Ca,149.246,0.036 +49Ti,42Ca,150.057,0.038 +49Ti,43Ca,149.615,0.037 +49Ti,44Ca,150.270,0.037 +49Ti,46Ca,149.609,0.110 +49Ti,48Ca,148.939,0.037 +49Ti,45Sc,76.431,0.036 +49Ti,46Ti,1.432,0.029 +49Ti,47Ti,0.952,0.025 +49Ti,48Ti,0.774,0.027 +50Ti,39K,220.470,0.041 +50Ti,41K,220.819,0.038 +50Ti,40Ca,149.408,0.031 +50Ti,42Ca,150.219,0.033 +50Ti,43Ca,149.777,0.032 +50Ti,44Ca,150.432,0.031 +50Ti,46Ca,149.771,0.109 +50Ti,48Ca,149.101,0.032 +50Ti,45Sc,76.593,0.032 +50Ti,46Ti,1.594,0.023 +50Ti,47Ti,1.114,0.022 +50Ti,48Ti,0.936,0.022 +51V,39K,299.083,0.041 +51V,41K,299.432,0.038 +51V,40Ca,228.021,0.036 +51V,42Ca,228.832,0.038 +51V,43Ca,228.390,0.036 +51V,44Ca,229.045,0.036 +51V,46Ca,228.384,0.110 +51V,48Ca,227.714,0.036 +51V,45Sc,155.206,0.035 +51V,46Ti,80.207,0.035 +51V,47Ti,79.727,0.034 +51V,48Ti,79.549,0.035 +50Cr,39K,378.060,0.042 +50Cr,41K,378.409,0.039 +50Cr,40Ca,306.998,0.037 +50Cr,42Ca,307.809,0.039 +50Cr,43Ca,307.367,0.038 +50Cr,44Ca,308.022,0.038 +50Cr,46Ca,307.361,0.111 +50Cr,48Ca,306.691,0.039 +50Cr,45Sc,234.183,0.037 +50Cr,46Ti,159.184,0.037 +50Cr,47Ti,158.704,0.035 +50Cr,48Ti,158.526,0.037 +52Cr,39K,379.168,0.038 +52Cr,41K,379.517,0.035 +52Cr,40Ca,308.106,0.033 +52Cr,42Ca,308.917,0.035 +52Cr,43Ca,308.475,0.033 +52Cr,44Ca,309.130,0.033 +52Cr,46Ca,308.469,0.110 +52Cr,48Ca,307.799,0.033 +52Cr,45Sc,235.291,0.032 +52Cr,46Ti,160.292,0.032 +52Cr,47Ti,159.812,0.030 +52Cr,48Ti,159.634,0.031 +53Cr,39K,378.263,0.041 +53Cr,41K,378.612,0.038 +53Cr,40Ca,307.201,0.035 +53Cr,42Ca,308.012,0.036 +53Cr,43Ca,307.570,0.035 +53Cr,44Ca,308.225,0.035 +53Cr,46Ca,307.564,0.110 +53Cr,48Ca,306.894,0.035 +53Cr,45Sc,234.386,0.035 +53Cr,46Ti,159.387,0.034 +53Cr,47Ti,158.907,0.033 +53Cr,48Ti,158.729,0.034 +54Cr,39K,376.770,0.045 +54Cr,41K,377.119,0.042 +54Cr,40Ca,305.708,0.035 +54Cr,42Ca,306.519,0.037 +54Cr,43Ca,306.077,0.036 +54Cr,44Ca,306.732,0.035 +54Cr,46Ca,306.071,0.111 +54Cr,48Ca,305.401,0.036 +54Cr,45Sc,232.893,0.035 +54Cr,46Ti,157.894,0.035 +54Cr,47Ti,157.414,0.033 +54Cr,48Ti,157.236,0.035 +55Mn,39K,459.736,0.046 +55Mn,41K,460.085,0.045 +55Mn,40Ca,388.674,0.035 +55Mn,42Ca,389.485,0.036 +55Mn,43Ca,389.043,0.035 +55Mn,44Ca,389.698,0.035 +55Mn,46Ca,389.037,0.110 +55Mn,48Ca,388.367,0.035 +55Mn,45Sc,315.859,0.031 +55Mn,46Ti,240.860,0.033 +55Mn,47Ti,240.380,0.030 +55Mn,48Ti,240.202,0.034 +56Fe,39K,543.924,0.041 +56Fe,41K,544.273,0.038 +56Fe,40Ca,472.862,0.035 +56Fe,42Ca,473.673,0.038 +56Fe,43Ca,473.231,0.037 +56Fe,44Ca,473.886,0.036 +56Fe,46Ca,473.225,0.110 +56Fe,48Ca,472.555,0.036 +56Fe,45Sc,400.047,0.036 +56Fe,46Ti,325.048,0.036 +56Fe,47Ti,324.568,0.035 +56Fe,48Ti,324.390,0.036 +56Fe,55Mn,84.188,0.029 +56Fe,54Cr,167.154,0.029 +56Fe,53Cr,165.661,0.033 +56Fe,52Cr,164.756,0.030 +56Fe,50Cr,165.864,0.032 +56Fe,51V,244.841,0.035 +56Fe,50Ti,323.454,0.035 +56Fe,49Ti,323.616,0.038 +55Mn,54Cr,82.966,0.028 +55Mn,53Cr,81.473,0.032 +55Mn,52Cr,80.568,0.029 +55Mn,50Cr,81.676,0.033 +55Mn,51V,160.653,0.034 +55Mn,50Ti,239.266,0.032 +55Mn,49Ti,239.428,0.035 +54Cr,53Cr,-1.493,0.022 +54Cr,52Cr,-2.398,0.020 +54Cr,50Cr,-1.290,0.027 +54Cr,51V,77.687,0.030 +54Cr,50Ti,156.300,0.031 +54Cr,49Ti,156.462,0.035 +53Cr,52Cr,-0.905,0.019 +53Cr,50Cr,0.203,0.028 +53Cr,51V,79.180,0.026 +53Cr,50Ti,157.793,0.030 +53Cr,49Ti,157.955,0.034 +52Cr,50Cr,1.108,0.022 +52Cr,51V,80.085,0.024 +52Cr,50Ti,158.698,0.027 +52Cr,49Ti,158.860,0.030 +50Cr,51V,78.977,0.031 +50Cr,50Ti,157.590,0.034 +50Cr,49Ti,157.752,0.036 +51V,50Ti,78.613,0.031 +51V,49Ti,78.775,0.034 +50Ti,49Ti,0.162,0.027 diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py b/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py new file mode 100644 index 0000000..0cb9915 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py @@ -0,0 +1,36 @@ +import csv + +from radbase.data_entry import (DataEntryInterface, + muonic_barret_theory_template, + muonic_transition_energy_difference_template, + muonic_transition_energy_template) + +ediff_values: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Transition': {'Upper': '2p3/2', 'Lower': '1s1/2'}, + 'Notes': 'Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ' +} + +bvalues: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Nuclear Polarization Method': 'Calculated', + 'Calculated Nuclear Polarization': [], + 'Notes': 'No theoretical uncertainties. #Exp_unc' +} + +interface = DataEntryInterface(start_interface=False) + +with open('./energy_diffs.csv', 'r') as f: + reader = list(csv.reader(f, delimiter=',')) + + for row in reader: + nuclideA, nuclideB, energy_diff, unc = row + + nuclideA = nuclideA[2:] + nuclideA[:2] + nuclideB = nuclideB[2:] + nuclideB[:2] + ediff_values['Nuclide_A'], ediff_values['Nuclide_B'] = nuclideA, nuclideB + + ediff_values['Energy Difference [keV] (A-B)'] = {'Value': energy_diff, + 'Uncertainty': unc} + + interface.save_data(muonic_transition_energy_difference_template, ediff_values, replacement_strategy='AlwaysReplace') diff --git a/radbase/data_entry.py b/radbase/data_entry.py index f49a698..8b1b0fa 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -251,7 +251,7 @@ def __init__(self, key: str = 'Nuclide'): def process(self, widget: tk.Widget): raw = widget.get() - if re.match(r'[a-zA-Z]{2}\d{1,3}', raw) or re.match(r'[a-zA-Z]{2}nat', raw): + if re.match(r'[a-zA-Z]{1,2}\d{1,3}', raw) or re.match(r'[a-zA-Z]{1,2}nat', raw): return {self.key: raw} else: raise ValueError( @@ -929,13 +929,14 @@ class InputTemplate(NamedTuple): reference_field, FieldSpec("Nuclide A", NuclideProcessor(key="Nuclide_A")), FieldSpec("Nuclide B", NuclideProcessor(key="Nuclide_B")), - transition_field, + transition_or_level_field, FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor("Energy Difference [keV] (A-B)")), notes_field ], data_key=lambda values: '_'.join( [values['Reference'], 'muonic_difference', values['Nuclide_A'], values['Nuclide_B'], - values['Transition']['Upper'], values['Transition']['Lower']]) + *([values['Transition']['Upper'], values['Transition']['Lower']] if 'Transition' in values else [ + values['Level'], ])]) ) muonic_transition_energy_difference_diff_transition_template = InputTemplate( @@ -943,7 +944,11 @@ class InputTemplate(NamedTuple): fields=[ reference_field, nuclide_field, - FieldSpec("Transitions", VariableNumberProcessor(TransitionProcessor()), VariableNumberWidgetCreator(TransitionWidgetCreator()), + FieldSpec("Transitions", + VariableNumberProcessor(XORProcessor([TransitionProcessor(), CastProcessor(str, key='Level')]), ), + VariableNumberWidgetCreator(GroupedWidgetCreator(['Transition', 'Level'], + [TransitionWidgetCreator(), + DefaultWidgetCreator()])), hovertext='Enter the upper and lower levels of the atomic/muonic transition'), FieldSpec("Energy Difference [keV] (A-B)", NumberWithUncertaintyProcessor("Energy Difference [keV] (A-B)")), notes_field @@ -951,7 +956,8 @@ class InputTemplate(NamedTuple): data_key=lambda values: '_'.join( [values['Reference'], 'muonic_difference', values['Nuclide'], *list( - sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values.items() if 'Transition' in field_name.lower()], + sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values.items() if + 'Transition' in field_name.lower()], ()))]) ) @@ -980,7 +986,7 @@ def mu_nuc_pol_key(values): name="Muonic Barrett Moment", fields=[ reference_field, - FieldSpec("Data used as input", PreviousDataProcessor(), + FieldSpec("Data used as input", PreviousDataProcessor(key='Previous Muonic Measurements'), PreviousDataWidgetCreator(compilation_path=config['compilation_dir'], filter_regex='muonic.*_')), nuclide_field, @@ -999,6 +1005,31 @@ def mu_nuc_pol_key(values): values['Previous Muonic Measurements']]]) ) +muonic_barret_shift_template = InputTemplate( + name="Muonic Barrett Moment Difference", + fields=[ + reference_field, + FieldSpec("Data used as input", PreviousDataProcessor(), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'], + filter_regex='muonic.*_')), + FieldSpec("Nuclide A", NuclideProcessor(key="Nuclide_A")), + FieldSpec("Nuclide B", NuclideProcessor(key="Nuclide_B")), + FieldSpec('Rka (A-B) [fm]', NumberWithUncertaintyProcessor('Rka [fm]')), + FieldSpec('k [-]', CastProcessor(str, key='k [-]')), + FieldSpec('alpha [1/fm]', CastProcessor(str, key='alpha [1/fm]')), + FieldSpec('Cz [fm/keV]', CastProcessor(str, key='Cz [fm/keV]')), + FieldSpec('Nuclear Polarization Method', + NuclearPolarizationProcessor(), + NuclearPolarizationWidgetCreator(compilation_path=config['compilation_dir']), + hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'barrett_moment_difference', values['Nuclide_A'], values['Nuclide_B'], + *['-'.join(s.split('_')[-2:]) for s in + values['Previous Muonic Measurements']]]) +) + muonic_radius_template = InputTemplate( name="Muonic Radius", fields=[ @@ -1042,6 +1073,7 @@ def mu_nuc_pol_key(values): muonic_transition_energy_difference_diff_transition_template, muonic_nuclear_polarization_calculation_template, muonic_barret_theory_template, + muonic_barret_shift_template, muonic_radius_template, muonic_fermi_distribution_template] @@ -1463,7 +1495,7 @@ def save_data( with file.open("w", encoding="utf-8") as f: json.dump(data_to_write, f, indent=4) - print(f"Data successfully saved to {file}") + # print(f"Data successfully saved to {file}") @staticmethod def _next_available_key(base_key: str, existing: dict) -> str: From bca32f9e1c55030eecd2c04d2e74fea8adf00dc7 Mon Sep 17 00:00:00 2001 From: Hunter Date: Wed, 18 Feb 2026 11:24:20 -0500 Subject: [PATCH 07/11] Adding Wo81, Fr68 --- .../frosch_electron_1968/cross_sections.csv | 173 +++++++ .../frosch_electron_1968/cross_sections_a.csv | 42 ++ .../frosch_electron_1968/cross_sections_b.csv | 31 ++ .../frosch_electron_1968/cross_sections_c.csv | 15 + .../frosch_1968_process.py | 30 ++ .../test_test_1700/Muonic Barrett Moment.json | 19 + ...alculated Muonic Nuclear Polarization.json | 275 ++++++++++ .../Calculated QED Correction.json | 275 ++++++++++ .../Fermi Distribution.json | 485 ++++++++++++++++++ .../Muonic Barrett Moment.json | 464 +++++++++++++++++ ...nergy Difference (different nuclides).json | 14 - .../Muonic Transition Energy.json | 275 ++++++++++ .../wolfhahrt_nuclear_1981/barrett_info.csv | 21 + .../wolfhahrt_nuclear_1981/energy_diffs.csv | 1 - .../wolfhart_1981_process.py | 104 +++- radbase/data_entry.py | 48 +- 16 files changed, 2246 insertions(+), 26 deletions(-) create mode 100644 radbase/compilation/frosch_electron_1968/cross_sections.csv create mode 100644 radbase/compilation/frosch_electron_1968/cross_sections_a.csv create mode 100644 radbase/compilation/frosch_electron_1968/cross_sections_b.csv create mode 100644 radbase/compilation/frosch_electron_1968/cross_sections_c.csv create mode 100644 radbase/compilation/frosch_electron_1968/frosch_1968_process.py create mode 100644 radbase/compilation/test_test_1700/Muonic Barrett Moment.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Calculated Muonic Nuclear Polarization.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Calculated QED Correction.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Fermi Distribution.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Muonic Barrett Moment.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy.json create mode 100644 radbase/compilation/wolfhahrt_nuclear_1981/barrett_info.csv diff --git a/radbase/compilation/frosch_electron_1968/cross_sections.csv b/radbase/compilation/frosch_electron_1968/cross_sections.csv new file mode 100644 index 0000000..f5bc6d0 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections.csv @@ -0,0 +1,173 @@ +Energy [keV],theta,Value,Quantity +250.0,32.0,(6.34±0.45)(2)ᵇ,Ca40 +250.0,32.0,(6.34±0.45)(2)ᵇ,Ca40 +250.0,35.0,(2.77±0.20)(2)ᵇ,Ca40 +250.0,37.5,(1.40±0.10)(2)ᵇ,Ca40 +250.0,40.0,(5.89±0.35)(1),Ca40 +250.0,42.0,(3.25±0.30)(1),Ca40 +250.0,44.0,(1.61±0.10)(1),Ca40 +250.0,46.0,(7.95±0.80)(0),Ca40 +250.0,47.0,(5.32±0.50)(0),Ca40 +250.0,48.0,(3.46±0.25)(0),Ca40 +250.0,49.0,(2.40±0.25)(0),Ca40 +250.0,50.0,(1.62±0.15)(0),Ca40 +250.0,51.0,(1.19±0.10)(0),Ca40 +250.0,52.0,(8.27±0.40)(−1),Ca40 +250.0,54.0,(5.38±0.40)(−1),Ca40 +250.0,55.0,(4.71±0.50)(−1),Ca40 +250.0,56.0,(4.32±0.30)(−1),Ca40 +250.0,58.0,(4.50±0.45)(−1),Ca40 +250.0,60.0,(4.82±0.30)(−1),Ca40 +250.0,64.0,(4.54±0.30)(−1),Ca40 +250.0,68.0,(3.24±0.25)(−1),Ca40 +250.0,72.0,(2.11±0.15)(−1),Ca40 +250.0,76.0,(1.18±0.10)(−1),Ca40 +250.0,80.0,(6.12±0.40)(−2),Ca40 +250.0,85.0,(2.23±0.15)(−2),Ca40 +250.0,90.0,(6.50±0.45)(−3),Ca40 +250.0,95.0,(1.42±0.10)(−3),Ca40 +250.0,100.0,(2.70±0.35)(−4),Ca40 +250.0,105.0,(2.13±0.25)(−4),Ca40 +250.0,110.0,(3.92±0.45)(−4),Ca40 +250.0,115.0,(3.13±0.55)(−4),Ca40 +250.0,125.0,(2.21±0.30)(−4),Ca40 +250.0,32.0,1.1±1.0ᶜ,D(Ca40-Ca48) +250.0,32.0,1.3±1.0ᵃ,D(Ca40-Ca48) +250.0,35.0,0.5±1.0ᶜ,D(Ca40-Ca48) +250.0,35.0,4.9±1.5ᵃ,D(Ca40-Ca48) +250.0,35.0,0.7±1.0ᶜ,D(Ca40-Ca48) +250.0,37.5,2.9±1.4,D(Ca40-Ca48) +250.0,37.5,3.2±1.0,D(Ca40-Ca48) +250.0,40.0,6.0±1.5,D(Ca40-Ca48) +250.0,42.0,4.9±1.0,D(Ca40-Ca48) +250.0,44.0,9.6±1.0,D(Ca40-Ca48) +250.0,46.0,9.2±1.0,D(Ca40-Ca48) +250.0,46.0,11.7±1.4,D(Ca40-Ca48) +250.0,47.0,10.2±1.3,D(Ca40-Ca48) +250.0,48.0,11.6±1.0,D(Ca40-Ca48) +250.0,49.0,12.8±1.3,D(Ca40-Ca48) +250.0,50.0,11.3±1.2,D(Ca40-Ca48) +250.0,50.0,11.5±1.0,D(Ca40-Ca48) +250.0,51.0,7.5±1.0,D(Ca40-Ca48) +250.0,52.0,−0.3±1.0,D(Ca40-Ca48) +250.0,53.0,−4.6±1.0,D(Ca40-Ca48) +250.0,54.0,−12.9±1.9,D(Ca40-Ca48) +250.0,54.0,−13.2±1.6,D(Ca40-Ca48) +250.0,55.0,−17.6±2.1,D(Ca40-Ca48) +250.0,56.0,−19.7±1.7,D(Ca40-Ca48) +250.0,58.0,−24.0±1.7,D(Ca40-Ca48) +250.0,58.0,−21.3±2.2,D(Ca40-Ca48) +250.0,60.0,−22.6±1.7,D(Ca40-Ca48) +250.0,62.0,−19.7±1.5,D(Ca40-Ca48) +250.0,64.0,−18.9±1.5,D(Ca40-Ca48) +250.0,68.0,−16.2±1.5,D(Ca40-Ca48) +250.0,72.0,−13.0±1.3,D(Ca40-Ca48) +250.0,76.0,−12.1±1.5,D(Ca40-Ca48) +250.0,80.0,−7.2±1.5,D(Ca40-Ca48) +250.0,85.0,−4.8±1.4,D(Ca40-Ca48) +250.0,90.0,1.7±2.0,D(Ca40-Ca48) +250.0,95.0,17.9±3.0,D(Ca40-Ca48) +250.0,100.0,−20.4±12,D(Ca40-Ca48) +250.0,105.0,−52.7±11,D(Ca40-Ca48) +250.0,110.0,−25.0±8.0,D(Ca40-Ca48) +250.0,115.0,−48.9±13,D(Ca40-Ca48) +250.0,125.0,−30.4±11,D(Ca40-Ca48) +250.0,32.0,2.7±0.9ᵃ,D(Ca40-Ca42) +250.0,32.0,,D(Ca40-Ca42) +250.0,35.0,,D(Ca40-Ca42) +250.0,36.0,3.3±0.8ᵃ,D(Ca40-Ca42) +250.0,37.5,,D(Ca40-Ca42) +250.0,40.0,5.3±1.0ᵃ,D(Ca40-Ca42) +250.0,44.0,5.4±1.0ᵃ,D(Ca40-Ca42) +250.0,48.0,8.2±1.0,D(Ca40-Ca42) +250.0,50.0,8.5±1.5,D(Ca40-Ca42) +250.0,52.0,5.2±1.0,D(Ca40-Ca42) +250.0,54.0,0.4±1.4,D(Ca40-Ca42) +250.0,56.0,−2.9±1.5,D(Ca40-Ca42) +250.0,60.0,−1.0±1.0,D(Ca40-Ca42) +250.0,64.0,−0.4±1.3,D(Ca40-Ca42) +250.0,68.0,−0.1±1.3,D(Ca40-Ca42) +250.0,72.0,2.3±1.5,D(Ca40-Ca42) +250.0,76.0,3.9±1.5,D(Ca40-Ca42) +250.0,80.0,6.5±1.4,D(Ca40-Ca42) +250.0,84.0,10.3±2.4,D(Ca40-Ca42) +250.0,32.0,1.3±1.0ᵈ,D(Ca40-Ca44) +250.0,32.0,,D(Ca40-Ca44) +250.0,35.0,3.0±1.0ᵈ,D(Ca40-Ca44) +250.0,35.0,,D(Ca40-Ca44) +250.0,36.0,,D(Ca40-Ca44) +250.0,37.5,6.4±1.0ᵈ,D(Ca40-Ca44) +250.0,37.5,,D(Ca40-Ca44) +250.0,40.0,5.7±0.8,D(Ca40-Ca44) +250.0,42.0,6.1±1.0,D(Ca40-Ca44) +250.0,44.0,8.0±0.8,D(Ca40-Ca44) +250.0,46.0,8.7±1.0,D(Ca40-Ca44) +250.0,48.0,12.3±0.9,D(Ca40-Ca44) +250.0,50.0,9.1±0.9,D(Ca40-Ca44) +250.0,52.0,5.8±0.7,D(Ca40-Ca44) +250.0,54.0,−4.8±1.0,D(Ca40-Ca44) +250.0,56.0,−8.7±1.1,D(Ca40-Ca44) +250.0,60.0,−9.0±1.1,D(Ca40-Ca44) +250.0,64.0,−5.7±1.0,D(Ca40-Ca44) +250.0,68.0,−4.4±1.5,D(Ca40-Ca44) +250.0,72.0,−0.5±1.0,D(Ca40-Ca44) +250.0,76.0,0.3±1.5,D(Ca40-Ca44) +250.0,80.0,4.0±2.0,D(Ca40-Ca44) +250.0,84.0,,D(Ca40-Ca44) +250.0,85.0,5.6±2.4,D(Ca40-Ca44) +250.0,90.0,12.5±3.1,D(Ca40-Ca44) +250.0,32.0,0.4±1.0ᶜ,D(Ca48-Ti48) +250.0,32.0,1.3±1.2ᵃ,D(Ca48-Ti48) +250.0,35.0,2.7±1.1ᵉ,D(Ca48-Ti48) +250.0,35.0,−0.2±1.5ᵃ,D(Ca48-Ti48) +250.0,37.5,4.1±1.0ᶜ,D(Ca48-Ti48) +250.0,37.5,3.4±1.4,D(Ca48-Ti48) +250.0,40.0,4.3±0.7,D(Ca48-Ti48) +250.0,42.0,5.0±1.0,D(Ca48-Ti48) +250.0,44.0,5.4±0.8,D(Ca48-Ti48) +250.0,46.0,6.1±1.0,D(Ca48-Ti48) +250.0,48.0,3.4±1.0,D(Ca48-Ti48) +250.0,50.0,−7.2±0.7,D(Ca48-Ti48) +250.0,52.0,−16.1±1.5,D(Ca48-Ti48) +250.0,54.0,−19.3±1.5,D(Ca48-Ti48) +250.0,56.0,−19.9±1.5,D(Ca48-Ti48) +250.0,58.0,−16.1±1.4,D(Ca48-Ti48) +250.0,60.0,−10.5±1.2,D(Ca48-Ti48) +250.0,62.0,−7.4±1.2,D(Ca48-Ti48) +250.0,64.0,−4.8±1.2,D(Ca48-Ti48) +250.0,66.0,−1.1±1.5,D(Ca48-Ti48) +250.0,68.0,1.8±1.4,D(Ca48-Ti48) +250.0,70.0,4.0±1.4,D(Ca48-Ti48) +250.0,72.0,5.5±1.4,D(Ca48-Ti48) +250.0,74.0,11.4±2.0,D(Ca48-Ti48) +250.0,76.0,8.6±1.4,D(Ca48-Ti48) +250.0,80.0,17.5±1.4,D(Ca48-Ti48) +250.0,85.0,20.9±2.4,D(Ca48-Ti48) +250.0,90.0,34.9±3.0,D(Ca48-Ti48) +500.0,32.0,(1.68±0.12)(0)ᵃ,Ca40 +500.0,35.0,(8.40±0.60)(−1)ᵃ,Ca40 +500.0,38.0,(2.98±0.22)(−1)ᵃ,Ca40 +500.0,40.0,(1.26±0.09)(−1)ᵃ,Ca40 +500.0,42.0,(4.35±0.44)(−2)ᵃ,Ca40 +500.0,44.0,(9.83±0.64)(−3)ᵃ,Ca40 +500.0,46.0,(2.34±0.28)(−3)ᵃ,Ca40 +500.0,46.0,(2.66±0.23)(−3),Ca40 +500.0,48.0,(2.21±0.16)(−3),Ca40 +500.0,51.0,(3.50±0.22)(−3),Ca40 +500.0,54.0,(2.98±0.26)(−3),Ca40 +500.0,57.0,(1.85±0.22)(−3),Ca40 +500.0,60.0,(7.98±0.80)(−4),Ca40 +500.0,63.0,(2.58±0.41)(−4),Ca40 +500.0,32.0,−17.1±0.9ᵃ,D(Ca40-Ca48) +500.0,35.0,−13.6±1.0ᵃ,D(Ca40-Ca48) +500.0,38.0,7.6±1.0ᵃ,D(Ca40-Ca48) +500.0,40.0,1.7±1.1ᵃ,D(Ca40-Ca48) +500.0,42.0,6.8±1.7ᵃ,D(Ca40-Ca48) +500.0,44.0,17.1±2.6ᵃ,D(Ca40-Ca48) +500.0,46.0,−14.9±5.1ᵃ,D(Ca40-Ca48) +500.0,46.0,19.5±3.1,D(Ca40-Ca48) +500.0,48.0,−47.1±2.1,D(Ca40-Ca48) +500.0,51.0,−36.1±1.5,D(Ca40-Ca48) +500.0,54.0,−27.9±2.4,D(Ca40-Ca48) +500.0,57.0,18.4±4.2,D(Ca40-Ca48) +500.0,60.0,−11.7±5.2,D(Ca40-Ca48) diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_a.csv b/radbase/compilation/frosch_electron_1968/cross_sections_a.csv new file mode 100644 index 0000000..5046700 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_a.csv @@ -0,0 +1,42 @@ +Energy [keV],theta,Ca40,D(Ca40-Ca48) +250.0,32.0,(6.34±0.45)(2)ᵇ,1.1±1.0ᶜ +250.0,32.0,(6.34±0.45)(2)ᵇ,1.3±1.0ᵃ +250.0,35.0,(2.77±0.20)(2)ᵇ,0.5±1.0ᶜ +250.0,35.0,...,4.9±1.5ᵃ +250.0,35.0,...,0.7±1.0ᶜ +250.0,37.5,(1.40±0.10)(2)ᵇ,2.9±1.4 +250.0,37.5,...,3.2±1.0 +250.0,40.0,(5.89±0.35)(1),6.0±1.5 +250.0,42.0,(3.25±0.30)(1),4.9±1.0 +250.0,44.0,(1.61±0.10)(1),9.6±1.0 +250.0,46.0,(7.95±0.80)(0),9.2±1.0 +250.0,46.0,...,11.7±1.4 +250.0,47.0,(5.32±0.50)(0),10.2±1.3 +250.0,48.0,(3.46±0.25)(0),11.6±1.0 +250.0,49.0,(2.40±0.25)(0),12.8±1.3 +250.0,50.0,(1.62±0.15)(0),11.3±1.2 +250.0,50.0,...,11.5±1.0 +250.0,51.0,(1.19±0.10)(0),7.5±1.0 +250.0,52.0,(8.27±0.40)(−1),−0.3±1.0 +250.0,53.0,...,−4.6±1.0 +250.0,54.0,(5.38±0.40)(−1),−12.9±1.9 +250.0,54.0,...,−13.2±1.6 +250.0,55.0,(4.71±0.50)(−1),−17.6±2.1 +250.0,56.0,(4.32±0.30)(−1),−19.7±1.7 +250.0,58.0,(4.50±0.45)(−1),−24.0±1.7 +250.0,58.0,...,−21.3±2.2 +250.0,60.0,(4.82±0.30)(−1),−22.6±1.7 +250.0,62.0,...,−19.7±1.5 +250.0,64.0,(4.54±0.30)(−1),−18.9±1.5 +250.0,68.0,(3.24±0.25)(−1),−16.2±1.5 +250.0,72.0,(2.11±0.15)(−1),−13.0±1.3 +250.0,76.0,(1.18±0.10)(−1),−12.1±1.5 +250.0,80.0,(6.12±0.40)(−2),−7.2±1.5 +250.0,85.0,(2.23±0.15)(−2),−4.8±1.4 +250.0,90.0,(6.50±0.45)(−3),1.7±2.0 +250.0,95.0,(1.42±0.10)(−3),17.9±3.0 +250.0,100.0,(2.70±0.35)(−4),−20.4±12 +250.0,105.0,(2.13±0.25)(−4),−52.7±11 +250.0,110.0,(3.92±0.45)(−4),−25.0±8.0 +250.0,115.0,(3.13±0.55)(−4),−48.9±13 +250.0,125.0,(2.21±0.30)(−4),−30.4±11 diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_b.csv b/radbase/compilation/frosch_electron_1968/cross_sections_b.csv new file mode 100644 index 0000000..e25c5fb --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_b.csv @@ -0,0 +1,31 @@ +Energy [keV],theta,D(Ca40-Ca42),D(Ca40-Ca44),D(Ca48-Ti48) +250,32.0,2.7±0.9ᵃ,1.3±1.0ᵈ,0.4±1.0ᶜ +250,32.0,,,1.3±1.2ᵃ +250,35.0,...,3.0±1.0ᵈ,2.7±1.1ᵉ +250,35.0,,,−0.2±1.5ᵃ +250,36.0,3.3±0.8ᵃ,,... +250,37.5,...,6.4±1.0ᵈ,4.1±1.0ᶜ +250,37.5,,,3.4±1.4 +250,40.0,5.3±1.0ᵃ,5.7±0.8,4.3±0.7 +250,42.0,...,6.1±1.0,5.0±1.0 +250,44.0,5.4±1.0ᵃ,8.0±0.8,5.4±0.8 +250,46.0,...,8.7±1.0,6.1±1.0 +250,48.0,8.2±1.0,12.3±0.9,3.4±1.0 +250,50.0,8.5±1.5,9.1±0.9,−7.2±0.7 +250,52.0,5.2±1.0,5.8±0.7,−16.1±1.5 +250,54.0,0.4±1.4,−4.8±1.0,−19.3±1.5 +250,56.0,−2.9±1.5,−8.7±1.1,−19.9±1.5 +250,58.0,...,...,−16.1±1.4 +250,60.0,−1.0±1.0,−9.0±1.1,−10.5±1.2 +250,62.0,...,...,−7.4±1.2 +250,64.0,−0.4±1.3,−5.7±1.0,−4.8±1.2 +250,66.0,...,...,−1.1±1.5 +250,68.0,−0.1±1.3,−4.4±1.5,1.8±1.4 +250,70.0,...,...,4.0±1.4 +250,72.0,2.3±1.5,−0.5±1.0,5.5±1.4 +250,74.0,...,...,11.4±2.0 +250,76.0,3.9±1.5,0.3±1.5,8.6±1.4 +250,80.0,6.5±1.4,4.0±2.0,17.5±1.4 +250,84.0,10.3±2.4,,... +250,85.0,...,5.6±2.4,20.9±2.4 +250,90.0,...,12.5±3.1,34.9±3.0 diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_c.csv b/radbase/compilation/frosch_electron_1968/cross_sections_c.csv new file mode 100644 index 0000000..61f9f68 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_c.csv @@ -0,0 +1,15 @@ +Energy [keV],theta,Ca40,D(Ca40-Ca48) +500,32,(1.68±0.12)(0)ᵃ,−17.1±0.9ᵃ +500,35,(8.40±0.60)(−1)ᵃ,−13.6±1.0ᵃ +500,38,(2.98±0.22)(−1)ᵃ,7.6±1.0ᵃ +500,40,(1.26±0.09)(−1)ᵃ,1.7±1.1ᵃ +500,42,(4.35±0.44)(−2)ᵃ,6.8±1.7ᵃ +500,44,(9.83±0.64)(−3)ᵃ,17.1±2.6ᵃ +500,46,(2.34±0.28)(−3)ᵃ,−14.9±5.1ᵃ +500,46,(2.66±0.23)(−3),19.5±3.1 +500,48,(2.21±0.16)(−3),−47.1±2.1 +500,51,(3.50±0.22)(−3),−36.1±1.5 +500,54,(2.98±0.26)(−3),−27.9±2.4 +500,57,(1.85±0.22)(−3),18.4±4.2 +500,60,(7.98±0.80)(−4),−11.7±5.2 +500,63,(2.58±0.41)(−4),... diff --git a/radbase/compilation/frosch_electron_1968/frosch_1968_process.py b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py new file mode 100644 index 0000000..24ca468 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py @@ -0,0 +1,30 @@ +import pandas as pd + +dfa = pd.read_csv('./cross_sections_a.csv') +dfb = pd.read_csv('./cross_sections_b.csv') +dfc = pd.read_csv('./cross_sections_c.csv') + +default_angle_acceptance = 1.8 +angle_acceptances = {'ᵃ': 0.9, 'ᵇ': 0.3, 'ᶜ': 0.36, 'ᵈ': 0.2} + +if 'Energy [keV]' not in dfb.columns: + dfb.insert(loc=0, column='Energy [keV]', value=250) + dfb.to_csv('./cross_sections_b.csv', index=False) + +for_all_cols = ['Energy [keV]', 'theta'] + +by_quant_dfs = [] +for df in [dfa, dfb, dfc]: + for column in df.columns: + if column not in for_all_cols: + col_df = df[~df[column].isin(['', '...'])] + col_df = col_df[for_all_cols + [column]] + col_df.rename(columns={column: 'Value'}, inplace=True) + col_df['Quantity'] = column + by_quant_dfs.append(col_df) + +by_quant_dfs = pd.concat(by_quant_dfs) +by_quant_dfs.to_csv('./cross_sections.csv', index=False) + +for i, row in by_quant_dfs.iterrows(): + print(row) diff --git a/radbase/compilation/test_test_1700/Muonic Barrett Moment.json b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json new file mode 100644 index 0000000..99c0fa2 --- /dev/null +++ b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json @@ -0,0 +1,19 @@ +{ + "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2": { + "Reference": "test_test_1700", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" + ], + "Nuclide": "Pb203", + "Rka [fm]": { + "value": 100.0, + "uncertainty": 3.0 + }, + "k [-]": "1", + "alpha [1/fm]": "1", + "Cz [fm/keV]": "1", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [], + "Notes": "" + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Calculated Muonic Nuclear Polarization.json b/radbase/compilation/wolfhahrt_nuclear_1981/Calculated Muonic Nuclear Polarization.json new file mode 100644 index 0000000..e739174 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Calculated Muonic Nuclear Polarization.json @@ -0,0 +1,275 @@ +{ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "K39", + "Energy [keV]": { + "Value": 0.145, + "Uncertainty": 0.0435 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "K41", + "Energy [keV]": { + "Value": 0.15, + "Uncertainty": 0.045 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca40", + "Energy [keV]": { + "Value": 0.17, + "Uncertainty": 0.051000000000000004 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca42", + "Energy [keV]": { + "Value": 0.196, + "Uncertainty": 0.0588 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca43", + "Energy [keV]": { + "Value": 0.181, + "Uncertainty": 0.054299999999999994 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca44", + "Energy [keV]": { + "Value": 0.205, + "Uncertainty": 0.06149999999999999 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca46", + "Energy [keV]": { + "Value": 0.208, + "Uncertainty": 0.0624 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca48", + "Energy [keV]": { + "Value": 0.19, + "Uncertainty": 0.056999999999999995 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Sc45", + "Energy [keV]": { + "Value": 0.233, + "Uncertainty": 0.0699 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti46", + "Energy [keV]": { + "Value": 0.285, + "Uncertainty": 0.08549999999999999 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti47", + "Energy [keV]": { + "Value": 0.265, + "Uncertainty": 0.0795 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti48", + "Energy [keV]": { + "Value": 0.284, + "Uncertainty": 0.08519999999999998 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti49", + "Energy [keV]": { + "Value": 0.237, + "Uncertainty": 0.0711 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti50", + "Energy [keV]": { + "Value": 0.253, + "Uncertainty": 0.0759 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "V51", + "Energy [keV]": { + "Value": 0.296, + "Uncertainty": 0.08879999999999999 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr50", + "Energy [keV]": { + "Value": 0.392, + "Uncertainty": 0.1176 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr52", + "Energy [keV]": { + "Value": 0.353, + "Uncertainty": 0.1059 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr53", + "Energy [keV]": { + "Value": 0.342, + "Uncertainty": 0.10260000000000001 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr54", + "Energy [keV]": { + "Value": 0.386, + "Uncertainty": 0.1158 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Mn55", + "Energy [keV]": { + "Value": 0.396, + "Uncertainty": 0.1188 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Fe56", + "Energy [keV]": { + "Value": 0.459, + "Uncertainty": 0.1377 + }, + "Notes": "30% uncertainty assigned." + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Calculated QED Correction.json b/radbase/compilation/wolfhahrt_nuclear_1981/Calculated QED Correction.json new file mode 100644 index 0000000..3cd9dde --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Calculated QED Correction.json @@ -0,0 +1,275 @@ +{ + "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "K39", + "Energy [keV]": { + "Value": 5.324, + "Uncertainty": 1.5972 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "K41", + "Energy [keV]": { + "Value": 5.305, + "Uncertainty": 1.5915 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca40", + "Energy [keV]": { + "Value": 5.907, + "Uncertainty": 1.7721 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca42", + "Energy [keV]": { + "Value": 5.891, + "Uncertainty": 1.7672999999999999 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca43", + "Energy [keV]": { + "Value": 5.897, + "Uncertainty": 1.7691000000000001 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca44", + "Energy [keV]": { + "Value": 5.886, + "Uncertainty": 1.7658 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca46", + "Energy [keV]": { + "Value": 5.897, + "Uncertainty": 1.7691000000000001 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ca48", + "Energy [keV]": { + "Value": 5.905, + "Uncertainty": 1.7715 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Sc45", + "Energy [keV]": { + "Value": 6.489, + "Uncertainty": 1.9466999999999999 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti46", + "Energy [keV]": { + "Value": 7.093, + "Uncertainty": 2.1279 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti47", + "Energy [keV]": { + "Value": 7.099, + "Uncertainty": 2.1297 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti48", + "Energy [keV]": { + "Value": 7.103, + "Uncertainty": 2.1309 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti49", + "Energy [keV]": { + "Value": 7.113, + "Uncertainty": 2.1339 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Ti50", + "Energy [keV]": { + "Value": 7.114, + "Uncertainty": 2.1342 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "V51", + "Energy [keV]": { + "Value": 7.758, + "Uncertainty": 2.3274 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr50", + "Energy [keV]": { + "Value": 8.391, + "Uncertainty": 2.5173 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr52", + "Energy [keV]": { + "Value": 8.408, + "Uncertainty": 2.5223999999999998 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr53", + "Energy [keV]": { + "Value": 8.391, + "Uncertainty": 2.5173 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Cr54", + "Energy [keV]": { + "Value": 8.366, + "Uncertainty": 2.5098 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Mn55", + "Energy [keV]": { + "Value": 9.041, + "Uncertainty": 2.7123 + }, + "Notes": "30% uncertainty assigned." + }, + "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Nuclide": "Fe56", + "Energy [keV]": { + "Value": 9.715, + "Uncertainty": 2.9145 + }, + "Notes": "30% uncertainty assigned." + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Fermi Distribution.json b/radbase/compilation/wolfhahrt_nuclear_1981/Fermi Distribution.json new file mode 100644 index 0000000..f63b47e --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Fermi Distribution.json @@ -0,0 +1,485 @@ +{ + "wolfhahrt_nuclear_1981_fermi_K39": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "K39", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.5681, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_K41": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "K41", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.5956, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca40": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca40", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.6377, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca42": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca42", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.6858, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca43": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca43", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.6643, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca44": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca44", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.7015, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca46": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca46", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.6713, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ca48": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ca48", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.6393, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Sc45": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Sc45", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.7465, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ti46": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ti46", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.8401, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ti47": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ti47", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.823, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ti48": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ti48", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.8185, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ti49": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ti49", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.7892, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Ti50": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Ti50", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.7851, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_V51": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "V51", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.8307, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Cr50": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Cr50", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.9262, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Cr52": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Cr52", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.8962, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Cr53": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Cr53", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.9222, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Cr54": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Cr54", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.9661, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Mn55": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Mn55", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 3.9962, + "Uncertainty": null + } + }, + "wolfhahrt_nuclear_1981_fermi_Fe56": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "a [fm]": { + "Value": 0.55, + "Uncertainty": null + }, + "Notes": "a fixed, c varied to reproduce 2p3/2-1s1/2 energies.", + "Nuclide": "Fe56", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2" + ], + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2" + ], + "c [fm]": { + "Value": 4.0449, + "Uncertainty": null + } + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Barrett Moment.json b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Barrett Moment.json new file mode 100644 index 0000000..91af048 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Barrett Moment.json @@ -0,0 +1,464 @@ +{ + "wolfhahrt_nuclear_1981_barrett_moment_K39_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "K39", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4073, + "Uncertainty": 0.0016 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.064", + "Cz [fm/keV]": "-0.0499", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_K41_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "K41", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4293, + "Uncertainty": 0.0014 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.064", + "Cz [fm/keV]": "-0.0499", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca40_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca40", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4626, + "Uncertainty": 0.001 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca42_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca42", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.5016, + "Uncertainty": 0.0012 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca43_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca43", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4841, + "Uncertainty": 0.0011 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca44_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca44", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.5143, + "Uncertainty": 0.0011 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca46_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca46", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4898, + "Uncertainty": 0.0045 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ca48_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ca48", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.4639, + "Uncertainty": 0.0011 + }, + "k [-]": "2.114", + "alpha [1/fm]": "0.065", + "Cz [fm/keV]": "-0.0420", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Sc45_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Sc45", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.5505, + "Uncertainty": 0.001 + }, + "k [-]": "2.116", + "alpha [1/fm]": "0.066", + "Cz [fm/keV]": "-0.0356", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ti46_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ti46", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6261, + "Uncertainty": 0.0008 + }, + "k [-]": "2.118", + "alpha [1/fm]": "0.068", + "Cz [fm/keV]": "-0.0307", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ti47_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ti47", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.612, + "Uncertainty": 0.0008 + }, + "k [-]": "2.118", + "alpha [1/fm]": "0.068", + "Cz [fm/keV]": "-0.0307", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ti48_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ti48", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6083, + "Uncertainty": 0.0008 + }, + "k [-]": "2.118", + "alpha [1/fm]": "0.068", + "Cz [fm/keV]": "-0.0307", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ti49_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ti49", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.5843, + "Uncertainty": 0.001 + }, + "k [-]": "2.118", + "alpha [1/fm]": "0.068", + "Cz [fm/keV]": "-0.0307", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Ti50_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Ti50", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.5809, + "Uncertainty": 0.0008 + }, + "k [-]": "2.118", + "alpha [1/fm]": "0.068", + "Cz [fm/keV]": "-0.0307", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_V51_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "V51", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6173, + "Uncertainty": 0.0007 + }, + "k [-]": "2.116", + "alpha [1/fm]": "0.069", + "Cz [fm/keV]": "-0.0265", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Cr50_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Cr50", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6947, + "Uncertainty": 0.0006 + }, + "k [-]": "2.115", + "alpha [1/fm]": "0.071", + "Cz [fm/keV]": "-0.0232", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Cr52_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Cr52", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6698, + "Uncertainty": 0.0005 + }, + "k [-]": "2.115", + "alpha [1/fm]": "0.071", + "Cz [fm/keV]": "-0.0232", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Cr53_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Cr53", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.6914, + "Uncertainty": 0.0006 + }, + "k [-]": "2.115", + "alpha [1/fm]": "0.071", + "Cz [fm/keV]": "-0.0232", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Cr54_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Cr54", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.7278, + "Uncertainty": 0.0007 + }, + "k [-]": "2.115", + "alpha [1/fm]": "0.071", + "Cz [fm/keV]": "-0.0232", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Mn55_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Mn55", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.7527, + "Uncertainty": 0.0007 + }, + "k [-]": "2.120", + "alpha [1/fm]": "0.072", + "Cz [fm/keV]": "-0.0203", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2" + ] + }, + "wolfhahrt_nuclear_1981_barrett_moment_Fe56_2p3/2-1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Nuclear Polarization Method": "Calculated", + "Notes": "No NP or QED uncertainties included. #Exp_unc", + "Nuclide": "Fe56", + "Previous Muonic Measurements": [ + "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2" + ], + "Rka [fm]": { + "Value": 4.7921, + "Uncertainty": 0.0005 + }, + "k [-]": "2.121", + "alpha [1/fm]": "0.074", + "Cz [fm/keV]": "-0.0181", + "Calculated Nuclear Polarization": [ + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2" + ], + "Calculated QED": [ + "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2" + ] + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json index aa8cc27..3456ab5 100644 --- a/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json @@ -1,18 +1,4 @@ { - "wolfhahrt_nuclear_1981_muonic_difference_wRo_lumnCo_2p3/2_1s1/2": { - "Reference": "wolfhahrt_nuclear_1981", - "Transition": { - "Upper": "2p3/2", - "Lower": "1s1/2" - }, - "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", - "Nuclide_A": "wRo", - "Nuclide_B": "lumnCo", - "Energy Difference [keV] (A-B)": { - "Value": "Value", - "Uncertainty": "Uncertainty" - } - }, "wolfhahrt_nuclear_1981_muonic_difference_K41_K39_2p3/2_1s1/2": { "Reference": "wolfhahrt_nuclear_1981", "Transition": { diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy.json b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy.json new file mode 100644 index 0000000..f3c6519 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy.json @@ -0,0 +1,275 @@ +{ + "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "K39", + "Energy [keV]": { + "Value": 713.118, + "Uncertainty": 0.032 + } + }, + "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "K41", + "Energy [keV]": { + "Value": 712.769, + "Uncertainty": 0.028 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca40", + "Energy [keV]": { + "Value": 784.18, + "Uncertainty": 0.025 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca42", + "Energy [keV]": { + "Value": 783.369, + "Uncertainty": 0.029 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca43", + "Energy [keV]": { + "Value": 783.811, + "Uncertainty": 0.027 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca44", + "Energy [keV]": { + "Value": 783.156, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca46", + "Energy [keV]": { + "Value": 783.817, + "Uncertainty": 0.107 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ca48", + "Energy [keV]": { + "Value": 784.487, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Sc45", + "Energy [keV]": { + "Value": 856.995, + "Uncertainty": 0.028 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ti46", + "Energy [keV]": { + "Value": 931.994, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ti47", + "Energy [keV]": { + "Value": 932.474, + "Uncertainty": 0.025 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ti48", + "Energy [keV]": { + "Value": 932.652, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ti49", + "Energy [keV]": { + "Value": 933.426, + "Uncertainty": 0.033 + } + }, + "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Ti50", + "Energy [keV]": { + "Value": 933.588, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "V51", + "Energy [keV]": { + "Value": 1012.201, + "Uncertainty": 0.026 + } + }, + "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Cr50", + "Energy [keV]": { + "Value": 1091.178, + "Uncertainty": 0.027 + } + }, + "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Cr52", + "Energy [keV]": { + "Value": 1092.286, + "Uncertainty": 0.021 + } + }, + "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Cr53", + "Energy [keV]": { + "Value": 1091.381, + "Uncertainty": 0.025 + } + }, + "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Cr54", + "Energy [keV]": { + "Value": 1089.888, + "Uncertainty": 0.031 + } + }, + "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Mn55", + "Energy [keV]": { + "Value": 1172.854, + "Uncertainty": 0.034 + } + }, + "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2": { + "Reference": "wolfhahrt_nuclear_1981", + "Transition": { + "Upper": "2p3/2", + "Lower": "1s1/2" + }, + "Notes": "Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ", + "Nuclide": "Fe56", + "Energy [keV]": { + "Value": 1257.042, + "Uncertainty": 0.025 + } + } +} diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/barrett_info.csv b/radbase/compilation/wolfhahrt_nuclear_1981/barrett_info.csv new file mode 100644 index 0000000..554c6b2 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/barrett_info.csv @@ -0,0 +1,21 @@ +39K,713.118(32),0.145,5.324,3.5681,3.4378,2.114,0.064,-0.0499,4.4073(16),-0.2276,10.666(7) +41K,712.769(28),0.150,5.305,3.5956,3.4549,2.114,0.064,-0.0499,4.4293(14),-0.2276,10.767(6) +40Ca,784.180(25),0.170,5.907,3.6377,3.4813,2.114,0.065,-0.0420,4.4626(10),-0.1922,10.879(5) +42Ca,783.369(29),0.196,5.891,3.6858,3.5115,2.114,0.065,-0.0420,4.5016(12),-0.1922,11.057(6) +43Ca,783.811(27),0.181,5.897,3.6643,3.4980,2.114,0.065,-0.0420,4.4841(11),-0.1922,10.977(5) +44Ca,783.156(26),0.205,5.886,3.7015,3.5214,2.114,0.065,-0.0420,4.5143(11),-0.1922,11.116(5) +46Ca,783.817(107),0.208,5.897,3.6713,3.5024,2.114,0.065,-0.0420,4.4898(45),-0.1922,11.003(21) +48Ca,784.487(26),0.190,5.905,3.6393,3.4823,2.114,0.065,-0.0420,4.4639(11),-0.1922,10.884(5) +45Sc,856.995(28),0.233,6.489,3.7465,3.5498,2.116,0.066,-0.0356,4.5505(10),-0.1649,11.270(5) +46Ti,931.994(26),0.285,7.093,3.8401,3.6094,2.118,0.068,-0.0307,4.6261(8),-0.1419,11.563(4) +47Ti,932.474(25),0.265,7.099,3.8230,3.5984,2.118,0.068,-0.0307,4.6120(8),-0.1419,11.498(4) +48Ti,932.652(26),0.284,7.103,3.8185,3.5956,2.118,0.068,-0.0307,4.6083(8),-0.1419,11.481(4) +49Ti,933.426(33),0.237,7.113,3.7892,3.5770,2.118,0.068,-0.0307,4.5843(10),-0.1419,11.370(5) +50Ti,933.588(26),0.253,7.114,3.7851,3.5743,2.118,0.068,-0.0307,4.5809(8),-0.1419,11.354(4) +51V,1012.201(26),0.296,7.758,3.8307,3.6033,2.116,0.069,-0.0265,4.6173(7),-0.1219,11.448(3) +50Cr,1091.178(27),0.392,8.391,3.9262,3.6645,2.115,0.071,-0.0232,4.6947(6),-0.1063,11.698(3) +52Cr,1092.286(21),0.353,8.408,3.8962,3.6452,2.115,0.071,-0.0232,4.6698(5),-0.1063,11.584(2) +53Cr,1091.381(25),0.342,8.391,3.9222,3.6620,2.115,0.071,-0.0232,4.6914(6),-0.1063,11.683(3) +54Cr,1089.888(31),0.386,8.366,3.9661,3.6902,2.115,0.071,-0.0232,4.7278(7),-0.1063,11.850(3) +55Mn,1172.854(34),0.396,9.041,3.9962,3.7096,2.120,0.072,-0.0203,4.7527(7),-0.0945,11.999(3) +56Fe,1257.042(25),0.459,9.715,4.0449,3.7412,2.121,0.074,-0.0181,4.7921(5),-0.0834,12.102(2) diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv b/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv index 5056334..1a7a32a 100644 --- a/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv +++ b/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv @@ -1,4 +1,3 @@ -Row,Column,Value,Uncertainty 41K,39K,-0.349,0.024 40Ca,39K,71.062,0.041 40Ca,41K,71.411,0.038 diff --git a/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py b/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py index 0cb9915..9f14bd1 100644 --- a/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py +++ b/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py @@ -1,9 +1,14 @@ import csv -from radbase.data_entry import (DataEntryInterface, - muonic_barret_theory_template, - muonic_transition_energy_difference_template, - muonic_transition_energy_template) +from uncertainties import ufloat_fromstr + +from radbase.data_entry import ( + DataEntryInterface, muonic_barret_theory_template, + muonic_fermi_distribution_template, + muonic_nuclear_polarization_calculation_template, + muonic_qed_calculation_template, + muonic_transition_energy_difference_template, + muonic_transition_energy_template) ediff_values: dict = { 'Reference': 'wolfhahrt_nuclear_1981', @@ -11,11 +16,34 @@ 'Notes': 'Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ' } -bvalues: dict = { +e_values: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Transition': {'Upper': '2p3/2', 'Lower': '1s1/2'}, + 'Notes': 'Determined from least squares fitting. HF splitting and isotopic impurity corrected. 2p3/2-1s from CoM of 2p-1s and theoretical FS splitting. ' +} + +np_values: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Transition': {'Upper': '2p3/2', 'Lower': '1s1/2'}, +} + +qed_values: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Transition': {'Upper': '2p3/2', 'Lower': '1s1/2'}, +} + +b_values: dict = { + 'Reference': 'wolfhahrt_nuclear_1981', + 'Nuclear Polarization Method': 'Calculated', + 'Notes': 'No NP or QED uncertainties included. #Exp_unc' +} + +f_values: dict = { 'Reference': 'wolfhahrt_nuclear_1981', 'Nuclear Polarization Method': 'Calculated', - 'Calculated Nuclear Polarization': [], - 'Notes': 'No theoretical uncertainties. #Exp_unc' + 'a [fm]': {'Value': 0.55, + 'Uncertainty': None}, + 'Notes': 'a fixed, c varied to reproduce 2p3/2-1s1/2 energies.' } interface = DataEntryInterface(start_interface=False) @@ -34,3 +62,65 @@ 'Uncertainty': unc} interface.save_data(muonic_transition_energy_difference_template, ediff_values, replacement_strategy='AlwaysReplace') + +with open('barrett_info.csv', 'r') as f: + reader = list(csv.reader(f, delimiter=',')) + + for row in reader: + nuclide, energy, np, qed, c, r, k, alpha, cz, rka, *_ = row + + nuclide = nuclide[2:] + nuclide[:2] + energy = ufloat_fromstr(energy) + e_values['Nuclide'] = nuclide + e_values['Energy [keV]'] = {'Value': energy.n, + 'Uncertainty': energy.s} + + interface.save_data(muonic_transition_energy_template, + e_values, replacement_strategy='AlwaysReplace') + + np_values['Nuclide'] = nuclide + np_values['Energy [keV]'] = {'Value': float(np), + 'Uncertainty': float(np)*0.3} + np_values['Notes'] = '30% uncertainty assigned.' + + interface.save_data(muonic_nuclear_polarization_calculation_template, + np_values, replacement_strategy='AlwaysReplace') + + qed_values['Nuclide'] = nuclide + qed_values['Energy [keV]'] = {'Value': float(qed), + 'Uncertainty': float(qed)*0.3} + qed_values['Notes'] = '30% uncertainty assigned.' + + interface.save_data(muonic_qed_calculation_template, + qed_values, replacement_strategy='AlwaysReplace') + + b_values['Nuclide'] = nuclide + f_values['Nuclide'] = nuclide + + e_key = muonic_transition_energy_template.data_key(e_values) + b_values['Previous Muonic Measurements'] = [e_key] + f_values['Previous Muonic Measurements'] = [e_key] + + rka = ufloat_fromstr(rka) + b_values['Rka [fm]'] = {'Value': rka.n, + 'Uncertainty': rka.s} + b_values['k [-]'] = k + b_values['alpha [1/fm]'] = alpha + b_values['Cz [fm/keV]'] = cz + + muonic_np_key = muonic_nuclear_polarization_calculation_template.data_key(np_values) + b_values['Calculated Nuclear Polarization'] = [muonic_np_key] + f_values['Calculated Nuclear Polarization'] = [muonic_np_key] + + muonic_qed_key = muonic_qed_calculation_template.data_key(qed_values) + b_values['Calculated QED'] = [muonic_qed_key] + f_values['Calculated QED'] = [muonic_qed_key] + + interface.save_data(muonic_barret_theory_template, + b_values, replacement_strategy='AlwaysReplace') + + f_values['c [fm]'] = {'Value': float(c), + 'Uncertainty': None} + + interface.save_data(muonic_fermi_distribution_template, + f_values, replacement_strategy='AlwaysReplace') diff --git a/radbase/data_entry.py b/radbase/data_entry.py index 8b1b0fa..44389ad 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -37,10 +37,20 @@ class Reference: class ScrollableFrame(ttk.Frame): def __init__(self, container, *args, **kwargs): super().__init__(container, *args, **kwargs) + canvas = tk.Canvas(self) scrollbar = ttk.Scrollbar(self, orient="vertical", command=canvas.yview) + self.scrollable_frame = ttk.Frame(canvas) + # Create window and store ID + self.window_id = canvas.create_window( + (0, 0), + window=self.scrollable_frame, + anchor="nw" + ) + + # Update scrollregion when content changes self.scrollable_frame.bind( "", lambda e: canvas.configure( @@ -48,7 +58,11 @@ def __init__(self, container, *args, **kwargs): ) ) - canvas.create_window((0, 0), window=self.scrollable_frame, anchor="nw") + # KEY FIX: make inner frame track canvas width + canvas.bind( + "", + lambda e: canvas.itemconfig(self.window_id, width=e.width) + ) canvas.configure(yscrollcommand=scrollbar.set) @@ -529,7 +543,7 @@ def create_widget(self, frame, row) -> tk.Widget: # --- filter entry --- filter_var = tk.StringVar() filter_var.set(self.filter_regex) - filter_entry = ttk.Entry(container, width=40, textvariable=filter_var) + filter_entry = ttk.Entry(container, width=80, textvariable=filter_var) filter_entry.grid(row=0, column=0, columnspan=2, sticky="w") # --- scrollable checklist --- @@ -555,7 +569,7 @@ def create_widget(self, frame, row) -> tk.Widget: text=data_key, variable=var ) - check.pack(anchor="w") + check.pack(expand=True, fill='x') vars_by_key[data_key] = var checkbox_widgets[data_key] = check @@ -982,6 +996,27 @@ def mu_nuc_pol_key(values): ], data_key=mu_nuc_pol_key) + +def mu_nuc_pol_key(values): + if 'Transition' in values: + return '_'.join([values['Reference'], 'muonic_qed', values['Nuclide'], + values['Transition']['Upper'], values['Transition']['Lower']]) + else: + return '_'.join([values['Reference'], 'muonic_qed', values['Nuclide'], + values['Level']]) + + +muonic_qed_calculation_template = InputTemplate( + name="Calculated QED Correction", + fields=[ + reference_field, + nuclide_field, + transition_or_level_field, + FieldSpec("Energy [keV]", NumberWithUncertaintyProcessor("Energy [keV]")), + notes_field + ], + data_key=mu_nuc_pol_key) + muonic_barret_theory_template = InputTemplate( name="Muonic Barrett Moment", fields=[ @@ -1022,6 +1057,9 @@ def mu_nuc_pol_key(values): NuclearPolarizationProcessor(), NuclearPolarizationWidgetCreator(compilation_path=config['compilation_dir']), hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), + FieldSpec('QED Calculations Used', + PreviousDataProcessor(key='Calculated QED'), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'])), notes_field ], data_key=lambda values: '_'.join( @@ -1072,6 +1110,7 @@ def mu_nuc_pol_key(values): muonic_transition_energy_difference_template, muonic_transition_energy_difference_diff_transition_template, muonic_nuclear_polarization_calculation_template, + muonic_qed_calculation_template, muonic_barret_theory_template, muonic_barret_shift_template, muonic_radius_template, @@ -1113,7 +1152,7 @@ def __init__(self, if start_interface: self.root = tk.Tk() - self.root.geometry("600x500") + self.root.minsize(650, 500) self.root.title("Data Entry Interface") def _on_mousewheel(event): @@ -1195,6 +1234,7 @@ def display_input(self, template: InputTemplate): form_frame.pack(padx=10, pady=10, expand=True, fill='both') form_frame = form_frame.scrollable_frame + form_frame.columnconfigure(1, weight=1) for row, field in enumerate(template.fields): label = ttk.Label(form_frame, From 4d89970d36e42ed9892ba27031f9da3206a93c42 Mon Sep 17 00:00:00 2001 From: Hunter Date: Thu, 19 Feb 2026 14:34:06 -0500 Subject: [PATCH 08/11] #Enhancement, decoupling widget unpacking and data validation --- ...ectron Scattering Cross Section Ratio.json | 2228 +++++++++++++++++ .../Electron Scattering Cross Section.json | 926 +++++++ .../frosch_electron_1968/cross_sections.csv | 12 +- .../frosch_electron_1968/cross_sections_a.csv | 2 +- .../frosch_electron_1968/cross_sections_b.csv | 4 +- .../frosch_electron_1968/cross_sections_c.csv | 2 +- .../frosch_1968_process.py | 94 +- ...ectron Scattering Cross Section Ratio.json | 1514 +++++++++++ .../cross_section_ratios.csv | 25 + .../lightbody_1983_process.py | 41 + radbase/data_entry.py | 200 +- 11 files changed, 4977 insertions(+), 71 deletions(-) create mode 100644 radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json create mode 100644 radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section.json create mode 100644 radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json create mode 100644 radbase/compilation/lightbody_elastic_1983/cross_section_ratios.csv create mode 100644 radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py diff --git a/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json new file mode 100644 index 0000000..f669630 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json @@ -0,0 +1,2228 @@ +{ + "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=6.984e-01": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 0.6984279472969682, + "Uncertainty": 0.021255559589947286 + }, + "Energy [MeV]": { + "Value": 250.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 32.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Ca40", + "Nuclide_B": "Ca48", + "Cross section Ratio [fm^2/sr]": { + "Value": 0.013000000000000001, + "Uncertainty": 0.01 + } + }, + 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"frosch_electron_1968_electron_cross_section_Ca40_q=1.898e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 1.8984053399285274, + "Uncertainty": 0.04100405072802559 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 44.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.983, + "Uncertainty": 0.064 + }, + "Notes": "Angular acceptance: 0.90" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=1.980e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 1.9801201416035437, + "Uncertainty": 0.04070867662378906 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 46.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.266, + "Uncertainty": 0.023000000000000003 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.061e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.061231779501573, + "Uncertainty": 0.040400902262299136 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 48.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.22100000000000003, + "Uncertainty": 0.016 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.182e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.1817143089415763, + "Uncertainty": 0.03991619634397461 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 51.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.35000000000000003, + "Uncertainty": 0.022000000000000002 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.301e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.300701600373293, + "Uncertainty": 0.03940413385853442 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 54.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.298, + "Uncertainty": 0.026000000000000002 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.418e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.418112105850723, + "Uncertainty": 0.03886506574802798 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 57.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.185, + "Uncertainty": 0.022000000000000002 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.534e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.5338653580781973, + "Uncertainty": 0.0382993614628112 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.07980000000000001, + "Uncertainty": 0.008 + }, + "Notes": "Angular acceptance: 1.80" + }, + "frosch_electron_1968_electron_cross_section_Ca40_q=2.648e+00": { + "Reference": "frosch_electron_1968", + "q [1/fm]": { + "Value": 2.6478820255586437, + "Uncertainty": 0.037707408708343604 + }, + "Energy [MeV]": { + "Value": 500.0, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 63.0, + "Uncertainty": 1.0 + }, + "Nuclide": "Ca40", + "Cross section [fm^2/sr]": { + "Value": 0.025800000000000003, + "Uncertainty": 0.0040999999999999995 + }, + "Notes": "Angular acceptance: 1.80" + } +} diff --git a/radbase/compilation/frosch_electron_1968/cross_sections.csv b/radbase/compilation/frosch_electron_1968/cross_sections.csv index f5bc6d0..b67bb50 100644 --- a/radbase/compilation/frosch_electron_1968/cross_sections.csv +++ b/radbase/compilation/frosch_electron_1968/cross_sections.csv @@ -1,4 +1,4 @@ -Energy [keV],theta,Value,Quantity +Energy [MeV],theta,Value,Quantity 250.0,32.0,(6.34±0.45)(2)ᵇ,Ca40 250.0,32.0,(6.34±0.45)(2)ᵇ,Ca40 250.0,35.0,(2.77±0.20)(2)ᵇ,Ca40 @@ -73,10 +73,7 @@ Energy [keV],theta,Value,Quantity 250.0,115.0,−48.9±13,D(Ca40-Ca48) 250.0,125.0,−30.4±11,D(Ca40-Ca48) 250.0,32.0,2.7±0.9ᵃ,D(Ca40-Ca42) -250.0,32.0,,D(Ca40-Ca42) -250.0,35.0,,D(Ca40-Ca42) 250.0,36.0,3.3±0.8ᵃ,D(Ca40-Ca42) -250.0,37.5,,D(Ca40-Ca42) 250.0,40.0,5.3±1.0ᵃ,D(Ca40-Ca42) 250.0,44.0,5.4±1.0ᵃ,D(Ca40-Ca42) 250.0,48.0,8.2±1.0,D(Ca40-Ca42) @@ -92,12 +89,8 @@ Energy [keV],theta,Value,Quantity 250.0,80.0,6.5±1.4,D(Ca40-Ca42) 250.0,84.0,10.3±2.4,D(Ca40-Ca42) 250.0,32.0,1.3±1.0ᵈ,D(Ca40-Ca44) -250.0,32.0,,D(Ca40-Ca44) 250.0,35.0,3.0±1.0ᵈ,D(Ca40-Ca44) -250.0,35.0,,D(Ca40-Ca44) -250.0,36.0,,D(Ca40-Ca44) 250.0,37.5,6.4±1.0ᵈ,D(Ca40-Ca44) -250.0,37.5,,D(Ca40-Ca44) 250.0,40.0,5.7±0.8,D(Ca40-Ca44) 250.0,42.0,6.1±1.0,D(Ca40-Ca44) 250.0,44.0,8.0±0.8,D(Ca40-Ca44) @@ -113,12 +106,11 @@ Energy [keV],theta,Value,Quantity 250.0,72.0,−0.5±1.0,D(Ca40-Ca44) 250.0,76.0,0.3±1.5,D(Ca40-Ca44) 250.0,80.0,4.0±2.0,D(Ca40-Ca44) -250.0,84.0,,D(Ca40-Ca44) 250.0,85.0,5.6±2.4,D(Ca40-Ca44) 250.0,90.0,12.5±3.1,D(Ca40-Ca44) 250.0,32.0,0.4±1.0ᶜ,D(Ca48-Ti48) 250.0,32.0,1.3±1.2ᵃ,D(Ca48-Ti48) -250.0,35.0,2.7±1.1ᵉ,D(Ca48-Ti48) +250.0,35.0,2.7±1.1ᶜ,D(Ca48-Ti48) 250.0,35.0,−0.2±1.5ᵃ,D(Ca48-Ti48) 250.0,37.5,4.1±1.0ᶜ,D(Ca48-Ti48) 250.0,37.5,3.4±1.4,D(Ca48-Ti48) diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_a.csv b/radbase/compilation/frosch_electron_1968/cross_sections_a.csv index 5046700..86f052e 100644 --- a/radbase/compilation/frosch_electron_1968/cross_sections_a.csv +++ b/radbase/compilation/frosch_electron_1968/cross_sections_a.csv @@ -1,4 +1,4 @@ -Energy [keV],theta,Ca40,D(Ca40-Ca48) +Energy [MeV],theta,Ca40,D(Ca40-Ca48) 250.0,32.0,(6.34±0.45)(2)ᵇ,1.1±1.0ᶜ 250.0,32.0,(6.34±0.45)(2)ᵇ,1.3±1.0ᵃ 250.0,35.0,(2.77±0.20)(2)ᵇ,0.5±1.0ᶜ diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_b.csv b/radbase/compilation/frosch_electron_1968/cross_sections_b.csv index e25c5fb..ac53c19 100644 --- a/radbase/compilation/frosch_electron_1968/cross_sections_b.csv +++ b/radbase/compilation/frosch_electron_1968/cross_sections_b.csv @@ -1,7 +1,7 @@ -Energy [keV],theta,D(Ca40-Ca42),D(Ca40-Ca44),D(Ca48-Ti48) +Energy [MeV],theta,D(Ca40-Ca42),D(Ca40-Ca44),D(Ca48-Ti48) 250,32.0,2.7±0.9ᵃ,1.3±1.0ᵈ,0.4±1.0ᶜ 250,32.0,,,1.3±1.2ᵃ -250,35.0,...,3.0±1.0ᵈ,2.7±1.1ᵉ +250,35.0,...,3.0±1.0ᵈ,2.7±1.1ᶜ 250,35.0,,,−0.2±1.5ᵃ 250,36.0,3.3±0.8ᵃ,,... 250,37.5,...,6.4±1.0ᵈ,4.1±1.0ᶜ diff --git a/radbase/compilation/frosch_electron_1968/cross_sections_c.csv b/radbase/compilation/frosch_electron_1968/cross_sections_c.csv index 61f9f68..0441277 100644 --- a/radbase/compilation/frosch_electron_1968/cross_sections_c.csv +++ b/radbase/compilation/frosch_electron_1968/cross_sections_c.csv @@ -1,4 +1,4 @@ -Energy [keV],theta,Ca40,D(Ca40-Ca48) +Energy [MeV],theta,Ca40,D(Ca40-Ca48) 500,32,(1.68±0.12)(0)ᵃ,−17.1±0.9ᵃ 500,35,(8.40±0.60)(−1)ᵃ,−13.6±1.0ᵃ 500,38,(2.98±0.22)(−1)ᵃ,7.6±1.0ᵃ diff --git a/radbase/compilation/frosch_electron_1968/frosch_1968_process.py b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py index 24ca468..273e779 100644 --- a/radbase/compilation/frosch_electron_1968/frosch_1968_process.py +++ b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py @@ -1,23 +1,44 @@ +import re + import pandas as pd +from scipy.constants import c, electron_volt, hbar, pi +from uncertainties import ufloat, ufloat_fromstr +from uncertainties.umath import sin + +from radbase.data_entry import ( + DataEntryInterface, electron_scattering_cross_section_ratio_template, + electron_scattering_cross_section_template) + + +def angle_acceptance(quantity_str): + angle_acceptances = {'ᵃ': 0.9, 'ᵇ': 0.3, 'ᶜ': 0.36, 'ᵈ': 0.2} + if quantity_str[-1] in angle_acceptances: + return quantity_str[:-1], angle_acceptances[quantity_str[-1]] + else: + return quantity_str, 1.8 + + +def convert_value(quantity_str): + quantity_str = quantity_str.replace('−', '-') + if len(matches := re.findall(r'\([^)^(]*\)', quantity_str)) == 2: + value, exponent = matches + value = ufloat_fromstr(value[1:-1]) * 10 ** int(exponent[1:-1]) + else: + value = ufloat_fromstr(quantity_str) + return value + dfa = pd.read_csv('./cross_sections_a.csv') dfb = pd.read_csv('./cross_sections_b.csv') dfc = pd.read_csv('./cross_sections_c.csv') -default_angle_acceptance = 1.8 -angle_acceptances = {'ᵃ': 0.9, 'ᵇ': 0.3, 'ᶜ': 0.36, 'ᵈ': 0.2} - -if 'Energy [keV]' not in dfb.columns: - dfb.insert(loc=0, column='Energy [keV]', value=250) - dfb.to_csv('./cross_sections_b.csv', index=False) - -for_all_cols = ['Energy [keV]', 'theta'] +for_all_cols = ['Energy [MeV]', 'theta'] by_quant_dfs = [] for df in [dfa, dfb, dfc]: for column in df.columns: if column not in for_all_cols: - col_df = df[~df[column].isin(['', '...'])] + col_df = df[~(df[column].isin(['', '...',]) | df[column].isna())] col_df = col_df[for_all_cols + [column]] col_df.rename(columns={column: 'Value'}, inplace=True) col_df['Quantity'] = column @@ -26,5 +47,58 @@ by_quant_dfs = pd.concat(by_quant_dfs) by_quant_dfs.to_csv('./cross_sections.csv', index=False) +interface = DataEntryInterface(start_interface=False) + for i, row in by_quant_dfs.iterrows(): - print(row) + + if row['Value'] is None: + continue + + cs_values: dict = {'Reference': 'frosch_electron_1968'} + + theta, nrg = row['theta'], row['Energy [MeV]'] + theta = ufloat(theta, 1) + nrg_j = nrg * electron_volt * 10 ** 6 + p_i = nrg_j / c # Ultra-relativistic + q = 2 * p_i / hbar * sin(theta / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 + + cs_values['q [1/fm]'] = {'Value': q.n, + 'Uncertainty': q.s} + + cs_values['Energy [MeV]'] = {'Value': nrg, + 'Uncertainty': None} + cs_values['theta [deg]'] = {'Value': theta.n, + 'Uncertainty': theta.s} + + if 'D' in row['Quantity']: + cs_values['Nuclide_A'] = row['Quantity'][2:6] + cs_values['Nuclide_B'] = row['Quantity'][7:11] + cs_values['q [1/fm]'] = {'Value': q.n, + 'Uncertainty': q.s} + + dratio = row['Value'] + dratio, angular_acceptance = angle_acceptance(dratio) + dratio = convert_value(dratio) / 100 # convert from percent + ratio = (1 - dratio) / (1 + dratio) + + cs_values['Cross section Ratio [fm^2/sr]'] = {'Value': dratio.n, + 'Uncertainty': dratio.s} + + interface.save_data(electron_scattering_cross_section_ratio_template, cs_values, + replacement_strategy='AlwaysReplace') + + + else: + cs_values['Nuclide'] = row['Quantity'] + + cs = row['Value'] + cs, angular_acceptance = angle_acceptance(cs) + cs = convert_value(cs) + cs *= 100 # microbarn to fm^2 conversion + cs_values['Cross section [fm^2/sr]'] = {'Value': cs.n, + 'Uncertainty': cs.s} + + cs_values['Notes'] = (f'Angular acceptance: {angular_acceptance:0.2f}') + + interface.save_data(electron_scattering_cross_section_template, cs_values, + replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json b/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json new file mode 100644 index 0000000..affc936 --- /dev/null +++ b/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json @@ -0,0 +1,1514 @@ +{ + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=1.520e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.15203192148469183, + "Uncertainty": 0.0022979616877686717 + }, + "Energy [MeV]": { + "Value": 30, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9977, + "Uncertainty": 0.0053 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=1.520e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.15203192148469183, + "Uncertainty": 0.0022979616877686717 + }, + "Energy [MeV]": { + "Value": 30, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0019, + "Uncertainty": 0.0058 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=1.520e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.15203192148469183, + "Uncertainty": 0.0022979616877686717 + }, + "Energy [MeV]": { + "Value": 30, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9995, + "Uncertainty": 0.0031 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=1.774e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.17737057506547382, + "Uncertainty": 0.0026809553023967843 + }, + "Energy [MeV]": { + "Value": 35, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0108, + "Uncertainty": 0.0057 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=1.774e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.17737057506547382, + "Uncertainty": 0.0026809553023967843 + }, + "Energy [MeV]": { + "Value": 35, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9896, + "Uncertainty": 0.0055 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=1.774e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.17737057506547382, + "Uncertainty": 0.0026809553023967843 + }, + "Energy [MeV]": { + "Value": 35, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0003, + "Uncertainty": 0.003 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.027e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.2027092286462558, + "Uncertainty": 0.003063948917024896 + }, + "Energy [MeV]": { + "Value": 40, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0046, + "Uncertainty": 0.0088 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.027e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.2027092286462558, + "Uncertainty": 0.003063948917024896 + }, + "Energy [MeV]": { + "Value": 40, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9903, + "Uncertainty": 0.0059 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=2.027e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.2027092286462558, + "Uncertainty": 0.003063948917024896 + }, + "Energy [MeV]": { + "Value": 40, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9949, + "Uncertainty": 0.0054 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.280e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.22804788222703773, + "Uncertainty": 0.0034469425316530074 + }, + "Energy [MeV]": { + "Value": 45, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0025, + "Uncertainty": 0.0061 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.280e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.22804788222703773, + "Uncertainty": 0.0034469425316530074 + }, + "Energy [MeV]": { + "Value": 45, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 60.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9919, + "Uncertainty": 0.0058 + } + }, + 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"lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=3.950e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.394990518575713, + "Uncertainty": 0.001990093198531034 + }, + "Energy [MeV]": { + "Value": 45, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9902, + "Uncertainty": 0.0035 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=4.389e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.43887835397301456, + "Uncertainty": 0.0022112146650344828 + }, + "Energy [MeV]": { + "Value": 50, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0172, + "Uncertainty": 0.0055 + } + }, + 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"lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=4.828e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.4827661893703159, + "Uncertainty": 0.0024323361315379314 + }, + "Energy [MeV]": { + "Value": 55, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.021, + "Uncertainty": 0.0059 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=4.828e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.4827661893703159, + "Uncertainty": 0.0024323361315379314 + }, + "Energy [MeV]": { + "Value": 55, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.961, + "Uncertainty": 0.0054 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=4.828e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.4827661893703159, + "Uncertainty": 0.0024323361315379314 + }, + "Energy [MeV]": { + "Value": 55, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9811, + "Uncertainty": 0.0037 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=5.267e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5266540247676172, + "Uncertainty": 0.002653457598041379 + }, + "Energy [MeV]": { + "Value": 60, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0206, + "Uncertainty": 0.0075 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=5.267e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5266540247676172, + "Uncertainty": 0.002653457598041379 + }, + "Energy [MeV]": { + "Value": 60, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9495, + "Uncertainty": 0.007 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=5.267e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5266540247676172, + "Uncertainty": 0.002653457598041379 + }, + "Energy [MeV]": { + "Value": 60, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.969, + "Uncertainty": 0.005 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=5.705e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5705418601649188, + "Uncertainty": 0.002874579064544828 + }, + "Energy [MeV]": { + "Value": 65, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0188, + "Uncertainty": 0.0071 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=5.705e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5705418601649188, + "Uncertainty": 0.002874579064544828 + }, + "Energy [MeV]": { + "Value": 65, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.943, + "Uncertainty": 0.0056 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=5.705e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.5705418601649188, + "Uncertainty": 0.002874579064544828 + }, + "Energy [MeV]": { + "Value": 65, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9608, + "Uncertainty": 0.0041 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=6.144e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6144296955622203, + "Uncertainty": 0.003095700531048276 + }, + "Energy [MeV]": { + "Value": 70, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0174, + "Uncertainty": 0.0085 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=6.144e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6144296955622203, + "Uncertainty": 0.003095700531048276 + }, + "Energy [MeV]": { + "Value": 70, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9348, + "Uncertainty": 0.0084 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=6.144e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6144296955622203, + "Uncertainty": 0.003095700531048276 + }, + "Energy [MeV]": { + "Value": 70, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9511, + "Uncertainty": 0.0053 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=6.583e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6583175309595217, + "Uncertainty": 0.0033168219975517246 + }, + "Energy [MeV]": { + "Value": 75, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0272, + "Uncertainty": 0.0068 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=6.583e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6583175309595217, + "Uncertainty": 0.0033168219975517246 + }, + "Energy [MeV]": { + "Value": 75, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9254, + "Uncertainty": 0.0057 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=6.583e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.6583175309595217, + "Uncertainty": 0.0033168219975517246 + }, + "Energy [MeV]": { + "Value": 75, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9505, + "Uncertainty": 0.0038 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=7.022e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7022053663568232, + "Uncertainty": 0.0035379434640551728 + }, + "Energy [MeV]": { + "Value": 80, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0118, + "Uncertainty": 0.0074 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=7.022e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7022053663568232, + "Uncertainty": 0.0035379434640551728 + }, + "Energy [MeV]": { + "Value": 80, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9151, + "Uncertainty": 0.006 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=7.022e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7022053663568232, + "Uncertainty": 0.0035379434640551728 + }, + "Energy [MeV]": { + "Value": 80, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9259, + "Uncertainty": 0.0041 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=7.461e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7460932017541245, + "Uncertainty": 0.0037590649305586214 + }, + "Energy [MeV]": { + "Value": 85, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr52", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 1.0258, + "Uncertainty": 0.0088 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=7.461e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7460932017541245, + "Uncertainty": 0.0037590649305586214 + }, + "Energy [MeV]": { + "Value": 85, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr52", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.8989, + "Uncertainty": 0.0074 + } + }, + "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=7.461e-01": { + "Reference": "lightbody_elastic_1983", + "q [1/fm]": { + "Value": 0.7460932017541245, + "Uncertainty": 0.0037590649305586214 + }, + "Energy [MeV]": { + "Value": 85, + "Uncertainty": null + }, + "theta [deg]": { + "Value": 120.0, + "Uncertainty": 1.0 + }, + "Nuclide_A": "Cr54", + "Nuclide_B": "Cr50", + "Cross section Ratio (A/B) [fm^2/sr]": { + "Value": 0.9221, + "Uncertainty": 0.0035 + } + } +} diff --git a/radbase/compilation/lightbody_elastic_1983/cross_section_ratios.csv b/radbase/compilation/lightbody_elastic_1983/cross_section_ratios.csv new file mode 100644 index 0000000..7d4221d --- /dev/null +++ b/radbase/compilation/lightbody_elastic_1983/cross_section_ratios.csv @@ -0,0 +1,25 @@ +Energy [MeV],theta,Cr52/Cr50,Cr54/Cr52,Cr54/Cr50 +30,60,0.9977(53),1.0019(58),0.9995(31) +35,60,1.0108(57),0.9896(55),1.0003(30) +40,60,1.0046(88),0.9903(59),0.9949(54) +45,60,1.0025(61),0.9919(58),0.9944(35) +50,60,1.0091(67),0.9885(56),0.9975(40) +55,60,1.0028(64),0.9888(70),0.9916(44) +60,60,1.0155(75),0.9800(73),0.9952(44) +65,60,0.9993(68),0.9880(63),0.9873(39) +70,60,1.0057(70),0.9808(73),0.9864(46) +75,60,1.0059(64),0.9809(60),0.9867(36) +80,60,1.0052(95),0.9816(78),0.9867(46) +85,60,1.0071(72),0.9747(64),0.9816(41) +30,120,0.9946(56),1.0062(58),1.0008(40) +35,120,0.9985(64),0.9891(67),0.9876(38) +40,120,1.0006(76),0.9864(67),0.9869(42) +45,120,1.0110(72),0.9794(68),0.9902(35) +50,120,1.0172(55),0.9587(57),0.9752(37) +55,120,1.0210(59),0.9610(54),0.9811(37) +60,120,1.0206(75),0.9495(70),0.9690(50) +65,120,1.0188(71),0.9430(56),0.9608(41) +70,120,1.0174(85),0.9348(84),0.9511(53) +75,120,1.0272(68),0.9254(57),0.9505(38) +80,120,1.0118(74),0.9151(60),0.9259(41) +85,120,1.0258(88),0.8989(74),0.9221(35) diff --git a/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py b/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py new file mode 100644 index 0000000..0df3f6b --- /dev/null +++ b/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py @@ -0,0 +1,41 @@ +import pandas as pd +from scipy.constants import c, electron_volt, hbar, pi +from uncertainties import ufloat, ufloat_fromstr +from uncertainties.umath import sin + +from radbase.data_entry import ( + DataEntryInterface, electron_scattering_cross_section_ratio_template) + +interface = DataEntryInterface(start_interface=False) + +df = pd.read_csv('./cross_section_ratios.csv') + +for i, row in df.iterrows(): + + theta, nrg = row['theta'], row['Energy [MeV]'] + theta = ufloat(theta, 1) + nrg_j = nrg * electron_volt * 10 ** 6 + p_i = nrg_j / c # Ultra-relativistic + q = 2 * p_i / hbar * sin(theta / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 + + for col in ['Cr52/Cr50', 'Cr54/Cr52', 'Cr54/Cr50']: + cs_values: dict = {'Reference': 'lightbody_elastic_1983'} + + cs_values['q [1/fm]'] = {'Value': q.n, + 'Uncertainty': q.s} + + cs_values['Energy [MeV]'] = {'Value': nrg, + 'Uncertainty': None} + cs_values['theta [deg]'] = {'Value': theta.n, + 'Uncertainty': theta.s} + + cs_values['Nuclide_A'] = col[:4] + cs_values['Nuclide_B'] = col[5:] + + ratio = ufloat_fromstr(row[col]) + + cs_values['Cross section Ratio (A/B) [fm^2/sr]'] = {'Value': ratio.n, + 'Uncertainty': ratio.s} + + interface.save_data(electron_scattering_cross_section_ratio_template, cs_values, + replacement_strategy='AlwaysReplace') diff --git a/radbase/data_entry.py b/radbase/data_entry.py index 44389ad..d88fe40 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -117,7 +117,14 @@ def _hide(self, _=None): class FieldProcessor(Protocol): + def process(self, widget: tk.Widget) -> dict[str, Any]: + return self.process_data(self.unpack_widget(widget)) + + def unpack_widget(self, widget: tk.Widget) -> Any: + pass + + def process_data(self, data: Any) -> dict[str, Any]: pass @@ -128,31 +135,43 @@ def __init__(self, field_type: type, key: str, allows_empty: bool = False): self.field_type = field_type self.allows_empty = allows_empty - def process(self, widget: tk.Widget): - raw = widget.get() - if raw == "" and not self.allows_empty: + def process(self, widget: tk.Widget) -> dict[str, Any]: + return self.process_data(self.unpack_widget(widget)) + + @staticmethod + def unpack_widget(widget: tk.Widget): + return widget.get() + + def process_data(self, data: str) -> dict[str, str]: + if data == "" and not self.allows_empty: raise ValueError("Field is empty") - return {self.key: self.field_type(raw)} + return {self.key: self.field_type(data)} class GroupedProcessor: - def __init__(self, processors: list[FieldProcessor]): + def __init__(self, processors: list[FieldProcessor], allows_empty=False): self.processors = processors + self.allows_empty = allows_empty - def process(self, widget: tk.Widget, allows_empty=False): - result = {} + def process(self, widget: tk.Widget): + return self.process_data(self.unpack_widget(widget)) - for sub_widget, processor in zip(widget.widgets, self.processors): + def unpack_widget(self, widget: tk.Widget): + return [processor.unpack_widget(sub_widget) for sub_widget, processor in zip(widget.widgets, self.processors)] + + def process_data(self, data: list): + result = {} + for sub_data, processor in zip(data, self.processors): try: - sub_result = processor.process(sub_widget) + sub_result = processor.process_data(sub_data) except ValueError: continue result = result | sub_result - if result == {} and not allows_empty: - raise ValueError(f'At least one sub_widget of {widget} must be non-empty for GroupedProcessor') + if result == {} and not self.allows_empty: + raise ValueError('At least one sub_widget must be non-empty for GroupedProcessor') return result @@ -163,15 +182,20 @@ def __init__(self, processors: list[FieldProcessor]): self.processors = processors def process(self, widget: tk.Widget): - result = {} + return self.process_data(self.unpack_widget(widget)) + def unpack_widget(self, widget: tk.Widget) -> list: if len(widget.widgets) != 2: raise ValueError('XOR processor applied to widget that does not have two fields.') + return [processor.unpack_widget(sub_widget) for sub_widget, processor in zip(widget.widgets, self.processors)] + + def process_data(self, data: list) -> dict[str, Any]: + result = {} num_filled = 0 - for sub_widget, processor in zip(widget.widgets, self.processors): + for sub_data, processor in zip(data, self.processors): try: - sub_result = processor.process(sub_widget) + sub_result = processor.process_data(sub_data) except ValueError: continue @@ -190,29 +214,29 @@ def __init__(self, key: str): self.key = key def process(self, widget: tk.Widget): - raw = widget.get().strip() + return self.process_data(self.unpack_widget(widget)) + + def process_data(self, data): try: - value = float(raw) + value = float(data) return {self.key: {'value': value, 'uncertainty': None}} except ValueError: try: - uvar = uncertainties.ufloat_fromstr(raw) + uvar = uncertainties.ufloat_fromstr(data) return {self.key: {'value': uvar.n, 'uncertainty': uvar.s}} except ValueError: raise ValueError( - f'Entered value of {raw} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') - - -class NuclearPolarizationProcessor: + f'Entered value of {data} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') @staticmethod - def process(widget: tk.Widget): - selection = widget.selection - fit_widget = widget.fit_widget - prev_calced_widget = widget.prev_calced_widget + def unpack_widget(widget: tk.Widget): + return widget.get().strip() + - calced_processor = PreviousDataProcessor(key='Calculated Nuclear Polarization') - varied_processor = VariableNumberProcessor( +class NuclearPolarizationProcessor: + def __init__(self): + self.calced_processor = PreviousDataProcessor(key='Calculated Nuclear Polarization') + self.varied_processor = VariableNumberProcessor( GroupedProcessor([ XORProcessor( [TransitionProcessor(), CastProcessor(str, key='Level')] @@ -220,15 +244,32 @@ def process(widget: tk.Widget): NumberWithUncertaintyProcessor('Energy [keV]') ])) + def process(self, widget: tk.Widget): + return self.process_data(self.unpack_widget(widget)) + + def unpack_widget(self, widget: tk.Widget) -> dict[str, Any]: + selection = widget.selection + fit_widget = widget.fit_widget + prev_calced_widget = widget.prev_calced_widget + mode = selection.get() - result = {'Nuclear Polarization Method': mode} + return {'mode': mode, + 'fit_data': self.varied_processor.unpack_widget(fit_widget), + 'calced_data': self.calced_processor.unpack_widget(prev_calced_widget)} + + def process_data(self, data): + mode = data['mode'] + fit_data = data['fit_data'] + calced_data = data['calced_data'] + + result = {'Nuclear Polarization Method': mode} if mode == 'Calculated': - return result | calced_processor.process(prev_calced_widget) + return result | self.calced_processor.process(calced_data) elif mode == 'Vary': - return result | varied_processor.process(fit_widget) + return result | self.varied_processor.process(fit_data) elif mode == 'Mixed': - return result | calced_processor.process(prev_calced_widget) | varied_processor.process(fit_widget) + return result | self.calced_processor.process(calced_data) | self.varied_processor.process(fit_data) else: raise ValueError(f'{mode} is not in [Calculated, Vary, Mixed]') @@ -239,10 +280,16 @@ def __init__(self, processor: FieldProcessor, suffixes: list[str] | None = None) self.processor = processor self.suffixes = suffixes if suffixes else [f'_{chr(ord('A') + i)}' for i in range(26)] - def process(self, widget: tk.Widget) -> dict: + def process(self, widget: tk.Widget): + return self.process_data(self.unpack_widget(widget)) + + def unpack_widget(self, widget: tk.Widget) -> list: + return [self.processor.unpack_widget(sub_widget) for sub_widget in widget.entries] + + def process_data(self, data): data = {} - for suffix, (label, widget) in zip(self.suffixes, widget.entries): - sub_result = self.processor.process(widget) + for suffix, sub_data in zip(self.suffixes, data): + sub_result = self.processor.process_data(sub_data) sub_result = {key + suffix: value for key, value in sub_result.items()} data = data | sub_result return data @@ -263,10 +310,16 @@ class NuclideProcessor: def __init__(self, key: str = 'Nuclide'): self.key = key - def process(self, widget: tk.Widget): - raw = widget.get() - if re.match(r'[a-zA-Z]{1,2}\d{1,3}', raw) or re.match(r'[a-zA-Z]{1,2}nat', raw): - return {self.key: raw} + def process(self, widget: tk.Widget) -> dict[str, str]: + return self.process_data(self.unpack_widget(widget)) + + @staticmethod + def unpack_widget(widget: tk.Widget): + return widget.get().strip() + + def process_data(self, data: str): + if re.match(r'[a-zA-Z]{1,2}\d{1,3}', data) or re.match(r'[a-zA-Z]{1,2}nat', data): + return {self.key: data} else: raise ValueError( 'Entered Nuclide does not match pattern of two letters and one to three numbers (Ex. Pb208') @@ -277,9 +330,16 @@ def __init__(self, key: str = 'Relies On'): self.key = key def process(self, widget: tk.Widget) -> dict[str, list[str]]: + return self.process_data(self.unpack_widget(widget)) + + @staticmethod + def unpack_widget(widget: tk.Widget): + return widget.selection_vars.items() + + def process_data(self, data: dict) -> dict[str, list[str]]: selected = [ key - for key, var in widget.selection_vars.items() + for key, var in data.items() if var.get() ] return {self.key: selected} @@ -299,15 +359,20 @@ def references(self): with open(self.reference_path, 'r') as f: return json.load(f) - def process(self, widget: tk.Widget): - value = widget.get().strip() + def process(self, widget: tk.Widget) -> dict[str, str]: + return self.process_data(self.unpack_widget(widget)) - if value not in sorted(self.references.keys()): + @staticmethod + def unpack_widget(widget: tk.Widget) -> str: + return widget.get().strip() + + def process_data(self, data: str): + if data not in sorted(self.references.keys()): raise ValueError( - f"Reference '{value}' is not a known citation key" + f"Reference '{data}' is not a known citation key" ) - return {self.key: value} + return {self.key: data} class SelectProcessor: @@ -355,8 +420,16 @@ def __init__(self, key: str = 'Transition'): self.key = key def process(self, widget: tk.Widget) -> dict[str, dict[str, str]]: - upper = widget.upper_entry.get().strip() - lower = widget.lower_entry.get().strip() + return self.process_data(self.unpack_widget(widget)) + + @staticmethod + def unpack_widget(widget: tk.Widget) -> dict[str, str]: + return {'Upper': widget.upper_entry.get().strip(), + 'Lower': widget.lower_entry.get().strip()} + + def process_data(self, data) -> dict[str, dict[str, str]]: + upper = data['Upper'] + lower = data['Lower'] if not upper or not lower: raise ValueError("Both upper and lower transition levels must be provided") @@ -1106,6 +1179,38 @@ def mu_nuc_pol_key(values): data_key=lambda values: '_'.join([values['Reference'], 'fermi', values['Nuclide']]) ) +electron_scattering_cross_section_template = InputTemplate( + name="Electron Scattering Cross Section", + fields=[ + reference_field, + nuclide_field, + FieldSpec('q [1/fm]', NumberWithUncertaintyProcessor(key='q [1/fm]')), + FieldSpec('E [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), + FieldSpec('theta [deg]', NumberWithUncertaintyProcessor(key='theta [deg]')), + FieldSpec('Cross section [μb/sr]', NumberWithUncertaintyProcessor(key='Cross section [μb/sr]')), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'electron_cross_section', values['Nuclide'], f'q={values['q [1/fm]']['Value']:0.3e}']) +) + +electron_scattering_cross_section_ratio_template = InputTemplate( + name="Electron Scattering Cross Section Ratio", + fields=[ + reference_field, + FieldSpec("Nuclide A", NuclideProcessor(key="Nuclide_A")), + FieldSpec("Nuclide B", NuclideProcessor(key="Nuclide_B")), + FieldSpec('q [1/fm]', NumberWithUncertaintyProcessor(key='q [1/fm]')), + FieldSpec('E [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), + FieldSpec('theta [deg]', NumberWithUncertaintyProcessor(key='theta [deg]')), + FieldSpec('Cross section Ratio (A/B) [μb/sr]', NumberWithUncertaintyProcessor(key='Cross section [μb/sr]')), + notes_field + ], + data_key=lambda values: '_'.join( + [values['Reference'], 'electron_cross_section_ratio', values['Nuclide_A'], values['Nuclide_B'], + f'q={values['q [1/fm]']['Value']:0.3e}']) +) + templates = [muonic_transition_energy_template, muonic_transition_energy_difference_template, muonic_transition_energy_difference_diff_transition_template, @@ -1114,7 +1219,8 @@ def mu_nuc_pol_key(values): muonic_barret_theory_template, muonic_barret_shift_template, muonic_radius_template, - muonic_fermi_distribution_template] + muonic_fermi_distribution_template, + electron_scattering_cross_section_template] class DataEntryInterface: From 0d0c2b9b89e78d06713f45abcdf802f424903071 Mon Sep 17 00:00:00 2001 From: Hunter Date: Sun, 22 Feb 2026 14:40:02 -0500 Subject: [PATCH 09/11] HOTFIX: Corrected NuclearPolarizationProcessor --- ...ectron Scattering Cross Section Ratio.json | 1484 +++---- .../Electron Scattering Cross Section.json | 528 +-- .../frosch_1968_process.py | 34 +- ...ectron Scattering Cross Section Ratio.json | 2354 +++++++++++ .../cross_section_ratios_198MeV.csv | 28 + .../cross_section_ratios_299p5MeV.csv | 34 + .../heisenberg_1972_process.py | 69 + ...ectron Scattering Cross Section Ratio.json | 864 ++-- .../Electron Scattering Cross Section.json | 3602 +++++++++++++++++ .../cross_section_Cr50.csv | 61 + .../cross_section_Cr52.csv | 63 + .../cross_section_Cr54.csv | 62 + .../lightbody_1983_process.py | 67 +- radbase/compilation/references.json | 98 + .../Muonic Transition Energy.json | 15 + .../Muonic Transition Energy.json | 28 + .../test_test_1700/Muonic Barrett Moment.json | 2601 ++++++++++++ .../Muonic Transition Energy.json | 13 + radbase/data_entry.py | 81 +- tests/test_data_entry.py | 38 +- 20 files changed, 10604 insertions(+), 1520 deletions(-) create mode 100644 radbase/compilation/heisenberg_electron_1972/Electron Scattering Cross Section Ratio.json create mode 100644 radbase/compilation/heisenberg_electron_1972/cross_section_ratios_198MeV.csv create mode 100644 radbase/compilation/heisenberg_electron_1972/cross_section_ratios_299p5MeV.csv create mode 100644 radbase/compilation/heisenberg_electron_1972/heisenberg_1972_process.py create mode 100644 radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section.json create mode 100644 radbase/compilation/lightbody_elastic_1983/cross_section_Cr50.csv create mode 100644 radbase/compilation/lightbody_elastic_1983/cross_section_Cr52.csv create mode 100644 radbase/compilation/lightbody_elastic_1983/cross_section_Cr54.csv create mode 100644 radbase/compilation/schaller_nuclear_1985/Muonic Transition Energy.json create mode 100644 radbase/compilation/tanaka_measurement_1984/Muonic Transition Energy.json diff --git a/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json index f669630..fcfffd2 100644 --- a/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json +++ b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section Ratio.json @@ -1,11 +1,11 @@ { - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=6.984e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=6.980e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.6984279472969682, - "Uncertainty": 0.021255559589947286 + "Value": 0.698, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -15,18 +15,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.013000000000000001, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.974, + "Uncertainty": 0.019 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=7.619e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=7.620e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.7619480083370856, - "Uncertainty": 0.021088729077864483 + "Value": 0.762, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -36,18 +36,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.006999999999999999, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.986, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=8.145e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.140e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.81448432585086, - "Uncertainty": 0.020938657891025794 + "Value": 0.814, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -57,18 +57,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.032, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.938, + "Uncertainty": 0.019 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=8.666e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.670e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.8666329929378521, - "Uncertainty": 0.020778621037064876 + "Value": 0.867, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -78,18 +78,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.06, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 0.887, + "Uncertainty": 0.027 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=9.081e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.080e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9080561327983517, - "Uncertainty": 0.020643467300597594 + "Value": 0.908, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -99,18 +99,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.049, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.907, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=9.492e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.490e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9492026699642637, - "Uncertainty": 0.020502025364012796 + "Value": 0.949, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -120,18 +120,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.096, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.825, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=9.901e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.900e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9900600708017718, - "Uncertainty": 0.02035433831189453 + "Value": 0.99, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -141,18 +141,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.11699999999999999, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.791, + "Uncertainty": 0.022 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.010e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.010e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.010376452315617, - "Uncertainty": 0.020278166851979997 + "Value": 1.01, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -162,18 +162,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.102, - "Uncertainty": 0.013000000000000001 + "Cross section Ratio [-]": { + "Value": 0.815, + "Uncertainty": 0.021 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.031e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.031e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0306158897507864, - "Uncertainty": 0.020200451131149568 + "Value": 1.031, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -183,18 +183,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.11599999999999999, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.792, + "Uncertainty": 0.016 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.051e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.051e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0507768417957601, - "Uncertainty": 0.020121197067756273 + "Value": 1.051, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -204,18 +204,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.128, - "Uncertainty": 0.013000000000000001 + "Cross section Ratio [-]": { + "Value": 0.773, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.071e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.071e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0708577731159827, - "Uncertainty": 0.02004041069730389 + "Value": 1.071, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -225,18 +225,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.115, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.794, + "Uncertainty": 0.016 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.091e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.091e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0908571544707881, - "Uncertainty": 0.019958098171987303 + "Value": 1.091, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -246,18 +246,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.075, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.86, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.111e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.111e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1107734628298558, - "Uncertainty": 0.019874265760223997 + "Value": 1.111, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -267,18 +267,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.003, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.006, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.131e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.131e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1306051814891944, - "Uncertainty": 0.019788919846176704 + "Value": 1.131, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -288,18 +288,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.046, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.096, + "Uncertainty": 0.022 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.150e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.150e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1503508001866465, - "Uncertainty": 0.01970206692926721 + "Value": 1.15, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -309,18 +309,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.132, - "Uncertainty": 0.016 + "Cross section Ratio [-]": { + "Value": 1.3, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.170e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.170e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1700088152169004, - "Uncertainty": 0.019613713623681386 + "Value": 1.17, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -330,18 +330,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.17600000000000002, - "Uncertainty": 0.021 + "Cross section Ratio [-]": { + "Value": 1.43, + "Uncertainty": 0.06 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.190e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.190e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1895777295460024, - "Uncertainty": 0.01952386665786555 + "Value": 1.19, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -351,18 +351,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.19699999999999998, - "Uncertainty": 0.017 + "Cross section Ratio [-]": { + "Value": 1.49, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.228e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.228e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2284423020052397, - "Uncertainty": 0.01933971922754796 + "Value": 1.228, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -372,18 +372,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.213, - "Uncertainty": 0.022000000000000002 + "Cross section Ratio [-]": { + "Value": 1.54, + "Uncertainty": 0.07 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.267e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.267e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2669326790390987, - "Uncertainty": 0.0191496807314056 + "Value": 1.267, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -393,18 +393,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.226, - "Uncertainty": 0.017 + "Cross section Ratio [-]": { + "Value": 1.58, + "Uncertainty": 0.06 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.305e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.305e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3050371361058701, - "Uncertainty": 0.01895380905700533 + "Value": 1.305, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -414,18 +414,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.19699999999999998, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.49, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.343e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.343e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3427440662188048, - "Uncertainty": 0.01875216386875662 + "Value": 1.343, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -435,18 +435,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.18899999999999997, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.47, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.417e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.417e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.416919526587691, - "Uncertainty": 0.01833180038298297 + "Value": 1.417, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -456,18 +456,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.162, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.39, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.489e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.489e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.4893686887731512, - "Uncertainty": 0.01788910242224003 + "Value": 1.489, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -477,18 +477,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.13, - "Uncertainty": 0.013000000000000001 + "Cross section Ratio [-]": { + "Value": 1.299, + "Uncertainty": 0.034 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.560e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.560e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5600032846310004, - "Uncertainty": 0.01742460934580058 + "Value": 1.56, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -498,18 +498,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.121, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.28, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.629e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.629e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6287372567866116, - "Uncertainty": 0.016938887066928577 + "Value": 1.629, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -519,18 +519,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.07200000000000001, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.155, + "Uncertainty": 0.035 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.712e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.712e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.711854623334179, - "Uncertainty": 0.01630278459352114 + "Value": 1.712, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -540,18 +540,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.048, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 1.101, + "Uncertainty": 0.031 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.792e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.792e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7917133773107732, - "Uncertainty": 0.01563564884305023 + "Value": 1.792, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -561,18 +561,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.017, - "Uncertainty": 0.02 + "Cross section Ratio [-]": { + "Value": 0.97, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.868e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.868e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.868161503039325, - "Uncertainty": 0.014938749746334384 + "Value": 1.868, + "Uncertainty": 0.015 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -582,18 +582,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.179, - "Uncertainty": 0.03 + "Cross section Ratio [-]": { + "Value": 0.7, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.941e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.941e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.9410534771674826, - "Uncertainty": 0.014213413890413367 + "Value": 1.941, + "Uncertainty": 0.014 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -603,18 +603,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.204, - "Uncertainty": 0.12 + "Cross section Ratio [-]": { + "Value": 1.5, + "Uncertainty": 0.4 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.010e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.010e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.0102505456795847, - "Uncertainty": 0.013461021993314311 + "Value": 2.01, + "Uncertainty": 0.013 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -624,18 +624,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.527, - "Uncertainty": 0.11 + "Cross section Ratio [-]": { + "Value": 3.2, + "Uncertainty": 1.0 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.076e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.076e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.075620988022814, - "Uncertainty": 0.012683006275776504 + "Value": 2.076, + "Uncertainty": 0.013 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -645,18 +645,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.25, - "Uncertainty": 0.08 + "Cross section Ratio [-]": { + "Value": 1.67, + "Uncertainty": 0.28 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.137e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.137e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.1370403678447563, - "Uncertainty": 0.011880847734937807 + "Value": 2.137, + "Uncertainty": 0.012 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -666,18 +666,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.489, - "Uncertainty": 0.13 + "Cross section Ratio [-]": { + "Value": 2.9, + "Uncertainty": 1.0 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.248e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.248e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.247566022430375, - "Uncertainty": 0.010210253051446426 + "Value": 2.248, + "Uncertainty": 0.01 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -687,18 +687,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.304, - "Uncertainty": 0.11 + "Cross section Ratio [-]": { + "Value": 1.9, + "Uncertainty": 0.5 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=6.984e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=6.980e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.6984279472969682, - "Uncertainty": 0.021255559589947286 + "Value": 0.698, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -708,18 +708,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.027000000000000003, - "Uncertainty": 0.009000000000000001 + "Cross section Ratio [-]": { + "Value": 0.947, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=7.830e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=7.830e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.7830074571041244, - "Uncertainty": 0.021029901161084497 + "Value": 0.783, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -729,18 +729,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.033, - "Uncertainty": 0.008 + "Cross section Ratio [-]": { + "Value": 0.936, + "Uncertainty": 0.015 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=8.666e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=8.670e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.8666329929378521, - "Uncertainty": 0.020778621037064876 + "Value": 0.867, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -750,18 +750,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.053, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.899, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=9.492e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=9.490e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9492026699642637, - "Uncertainty": 0.020502025364012796 + "Value": 0.949, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -771,18 +771,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.054000000000000006, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.898, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.031e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.031e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0306158897507864, - "Uncertainty": 0.020200451131149568 + "Value": 1.031, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -792,18 +792,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.08199999999999999, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.848, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.071e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.071e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0708577731159827, - "Uncertainty": 0.02004041069730389 + "Value": 1.071, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -813,18 +813,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.085, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 0.843, + "Uncertainty": 0.025 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.111e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.111e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1107734628298558, - "Uncertainty": 0.019874265760223997 + "Value": 1.111, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -834,18 +834,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.052000000000000005, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.901, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.150e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.150e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1503508001866465, - "Uncertainty": 0.01970206692926721 + "Value": 1.15, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -855,18 +855,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.004, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.992, + "Uncertainty": 0.028 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.190e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.190e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1895777295460024, - "Uncertainty": 0.01952386665786555 + "Value": 1.19, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -876,18 +876,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.028999999999999998, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.06, + "Uncertainty": 0.032 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.267e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.267e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2669326790390987, - "Uncertainty": 0.0191496807314056 + "Value": 1.267, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -897,18 +897,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.01, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.02, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.343e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.343e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3427440662188048, - "Uncertainty": 0.01875216386875662 + "Value": 1.343, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -918,18 +918,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.004, - "Uncertainty": 0.013000000000000001 + "Cross section Ratio [-]": { + "Value": 1.008, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.417e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.417e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.416919526587691, - "Uncertainty": 0.01833180038298297 + "Value": 1.417, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -939,18 +939,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.001, - "Uncertainty": 0.013000000000000001 + "Cross section Ratio [-]": { + "Value": 1.002, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.489e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.489e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.4893686887731512, - "Uncertainty": 0.01788910242224003 + "Value": 1.489, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -960,18 +960,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.023, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 0.955, + "Uncertainty": 0.029 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.560e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.560e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5600032846310004, - "Uncertainty": 0.01742460934580058 + "Value": 1.56, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -981,18 +981,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.039, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 0.925, + "Uncertainty": 0.028 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.629e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.629e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6287372567866116, - "Uncertainty": 0.016938887066928577 + "Value": 1.629, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1002,18 +1002,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.065, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.878, + "Uncertainty": 0.025 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca42_q=1.695e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.695e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.69548686348257, - "Uncertainty": 0.016432527363401055 + "Value": 1.695, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1023,18 +1023,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca42", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.10300000000000001, - "Uncertainty": 0.024 + "Cross section Ratio [-]": { + "Value": 0.81, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=6.984e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=6.980e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.6984279472969682, - "Uncertainty": 0.021255559589947286 + "Value": 0.698, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1044,18 +1044,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.013000000000000001, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.974, + "Uncertainty": 0.019 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=7.619e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=7.620e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.7619480083370856, - "Uncertainty": 0.021088729077864483 + "Value": 0.762, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1065,18 +1065,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.03, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.942, + "Uncertainty": 0.019 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=8.145e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.140e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.81448432585086, - "Uncertainty": 0.020938657891025794 + "Value": 0.814, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1086,18 +1086,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.064, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.88, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=8.666e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.670e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.8666329929378521, - "Uncertainty": 0.020778621037064876 + "Value": 0.867, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1107,18 +1107,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.057, - "Uncertainty": 0.008 + "Cross section Ratio [-]": { + "Value": 0.892, + "Uncertainty": 0.014 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=9.081e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.080e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9080561327983517, - "Uncertainty": 0.020643467300597594 + "Value": 0.908, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1128,18 +1128,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.061, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.885, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=9.492e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.490e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9492026699642637, - "Uncertainty": 0.020502025364012796 + "Value": 0.949, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1149,18 +1149,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.08, - "Uncertainty": 0.008 + "Cross section Ratio [-]": { + "Value": 0.852, + "Uncertainty": 0.014 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=9.901e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.900e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9900600708017718, - "Uncertainty": 0.02035433831189453 + "Value": 0.99, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1170,18 +1170,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.087, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.84, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.031e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.031e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0306158897507864, - "Uncertainty": 0.020200451131149568 + "Value": 1.031, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1191,18 +1191,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.12300000000000001, - "Uncertainty": 0.009000000000000001 + "Cross section Ratio [-]": { + "Value": 0.781, + "Uncertainty": 0.014 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.071e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.071e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0708577731159827, - "Uncertainty": 0.02004041069730389 + "Value": 1.071, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1212,18 +1212,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.091, - "Uncertainty": 0.009000000000000001 + "Cross section Ratio [-]": { + "Value": 0.833, + "Uncertainty": 0.015 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.111e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.111e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1107734628298558, - "Uncertainty": 0.019874265760223997 + "Value": 1.111, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1233,18 +1233,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.057999999999999996, - "Uncertainty": 0.006999999999999999 + "Cross section Ratio [-]": { + "Value": 0.89, + "Uncertainty": 0.013 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.150e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.150e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1503508001866465, - "Uncertainty": 0.01970206692926721 + "Value": 1.15, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1254,18 +1254,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.048, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.101, + "Uncertainty": 0.022 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.190e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.190e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1895777295460024, - "Uncertainty": 0.01952386665786555 + "Value": 1.19, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1275,18 +1275,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.087, - "Uncertainty": 0.011000000000000001 + "Cross section Ratio [-]": { + "Value": 1.191, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.267e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.267e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2669326790390987, - "Uncertainty": 0.0191496807314056 + "Value": 1.267, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1296,18 +1296,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.09, - "Uncertainty": 0.011000000000000001 + "Cross section Ratio [-]": { + "Value": 1.198, + "Uncertainty": 0.027 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.343e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.343e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3427440662188048, - "Uncertainty": 0.01875216386875662 + "Value": 1.343, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1317,18 +1317,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.057, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.121, + "Uncertainty": 0.022 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.417e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.417e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.416919526587691, - "Uncertainty": 0.01833180038298297 + "Value": 1.417, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1338,18 +1338,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.044000000000000004, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.092, + "Uncertainty": 0.033 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.489e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.489e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.4893686887731512, - "Uncertainty": 0.01788910242224003 + "Value": 1.489, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1359,18 +1359,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.005, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.01, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.560e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.560e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5600032846310004, - "Uncertainty": 0.01742460934580058 + "Value": 1.56, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1380,18 +1380,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.003, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 0.994, + "Uncertainty": 0.03 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.629e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.629e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6287372567866116, - "Uncertainty": 0.016938887066928577 + "Value": 1.629, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1401,18 +1401,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.04, - "Uncertainty": 0.02 + "Cross section Ratio [-]": { + "Value": 0.92, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.712e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.712e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.711854623334179, - "Uncertainty": 0.01630278459352114 + "Value": 1.712, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1422,18 +1422,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.055999999999999994, - "Uncertainty": 0.024 + "Cross section Ratio [-]": { + "Value": 0.89, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca44_q=1.792e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.792e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7917133773107732, - "Uncertainty": 0.01563564884305023 + "Value": 1.792, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1443,18 +1443,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca44", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.125, - "Uncertainty": 0.031000000000000003 + "Cross section Ratio [-]": { + "Value": 0.78, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=6.984e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=6.980e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.6984279472969682, - "Uncertainty": 0.021255559589947286 + "Value": 0.698, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1464,18 +1464,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.013000000000000001, - "Uncertainty": 0.012 + "Cross section Ratio [-]": { + "Value": 0.974, + "Uncertainty": 0.023 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=7.619e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=7.620e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.7619480083370856, - "Uncertainty": 0.021088729077864483 + "Value": 0.762, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1485,18 +1485,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.002, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.004, + "Uncertainty": 0.03 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=8.145e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.140e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.81448432585086, - "Uncertainty": 0.020938657891025794 + "Value": 0.814, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1506,18 +1506,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.034, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.934, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=8.666e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.670e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.8666329929378521, - "Uncertainty": 0.020778621037064876 + "Value": 0.867, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1527,18 +1527,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.043, - "Uncertainty": 0.006999999999999999 + "Cross section Ratio [-]": { + "Value": 0.918, + "Uncertainty": 0.013 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=9.081e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.080e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9080561327983517, - "Uncertainty": 0.020643467300597594 + "Value": 0.908, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1548,18 +1548,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.05, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.905, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=9.492e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.490e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9492026699642637, - "Uncertainty": 0.020502025364012796 + "Value": 0.949, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1569,18 +1569,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.054000000000000006, - "Uncertainty": 0.008 + "Cross section Ratio [-]": { + "Value": 0.898, + "Uncertainty": 0.014 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=9.901e-01": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.900e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9900600708017718, - "Uncertainty": 0.02035433831189453 + "Value": 0.99, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1590,18 +1590,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.061, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.885, + "Uncertainty": 0.018 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.031e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.031e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0306158897507864, - "Uncertainty": 0.020200451131149568 + "Value": 1.031, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1611,18 +1611,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.034, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.934, + "Uncertainty": 0.019 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.071e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.071e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0708577731159827, - "Uncertainty": 0.02004041069730389 + "Value": 1.071, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1632,18 +1632,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.07200000000000001, - "Uncertainty": 0.006999999999999999 + "Cross section Ratio [-]": { + "Value": 1.155, + "Uncertainty": 0.016 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.111e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.111e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1107734628298558, - "Uncertainty": 0.019874265760223997 + "Value": 1.111, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1653,18 +1653,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.161, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.38, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.150e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.150e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1503508001866465, - "Uncertainty": 0.01970206692926721 + "Value": 1.15, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1674,18 +1674,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.193, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.48, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.190e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.190e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1895777295460024, - "Uncertainty": 0.01952386665786555 + "Value": 1.19, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1695,18 +1695,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.19899999999999998, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.5, + "Uncertainty": 0.05 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.228e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.228e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2284423020052397, - "Uncertainty": 0.01933971922754796 + "Value": 1.228, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1716,18 +1716,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.161, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 1.38, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.267e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.267e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2669326790390987, - "Uncertainty": 0.0191496807314056 + "Value": 1.267, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1737,18 +1737,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.105, - "Uncertainty": 0.012 + "Cross section Ratio [-]": { + "Value": 1.235, + "Uncertainty": 0.03 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.305e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.305e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3050371361058701, - "Uncertainty": 0.01895380905700533 + "Value": 1.305, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1758,18 +1758,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.07400000000000001, - "Uncertainty": 0.012 + "Cross section Ratio [-]": { + "Value": 1.16, + "Uncertainty": 0.028 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.343e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.343e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3427440662188048, - "Uncertainty": 0.01875216386875662 + "Value": 1.343, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1779,18 +1779,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.048, - "Uncertainty": 0.012 + "Cross section Ratio [-]": { + "Value": 1.101, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.380e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.380e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3800419834817157, - "Uncertainty": 0.0185448065897372 + "Value": 1.38, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1800,18 +1800,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.011000000000000001, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 1.022, + "Uncertainty": 0.031 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.417e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.417e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.416919526587691, - "Uncertainty": 0.01833180038298297 + "Value": 1.417, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1821,18 +1821,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.018000000000000002, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.965, + "Uncertainty": 0.027 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.453e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.453e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.45336546227986, - "Uncertainty": 0.018113210132247946 + "Value": 1.453, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1842,18 +1842,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.04, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.923, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.489e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.489e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.4893686887731512, - "Uncertainty": 0.01788910242224003 + "Value": 1.489, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1863,18 +1863,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.055, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.896, + "Uncertainty": 0.025 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.525e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.525e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5249182391360037, - "Uncertainty": 0.017659545518338676 + "Value": 1.525, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1884,18 +1884,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.114, - "Uncertainty": 0.02 + "Cross section Ratio [-]": { + "Value": 0.795, + "Uncertainty": 0.032 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.560e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.560e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5600032846310004, - "Uncertainty": 0.01742460934580058 + "Value": 1.56, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1905,18 +1905,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.086, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.842, + "Uncertainty": 0.024 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.629e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.629e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6287372567866116, - "Uncertainty": 0.016938887066928577 + "Value": 1.629, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1926,18 +1926,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.175, - "Uncertainty": 0.013999999999999999 + "Cross section Ratio [-]": { + "Value": 0.702, + "Uncertainty": 0.02 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.712e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.712e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.711854623334179, - "Uncertainty": 0.01630278459352114 + "Value": 1.712, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1947,18 +1947,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.209, - "Uncertainty": 0.024 + "Cross section Ratio [-]": { + "Value": 0.654, + "Uncertainty": 0.033 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca48_Ti48_q=1.792e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.792e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7917133773107732, - "Uncertainty": 0.01563564884305023 + "Value": 1.792, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -1968,18 +1968,18 @@ }, "Nuclide_A": "Ca48", "Nuclide_B": "Ti48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.349, - "Uncertainty": 0.03 + "Cross section Ratio [-]": { + "Value": 0.483, + "Uncertainty": 0.033 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.397e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.400e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3968558945939364, - "Uncertainty": 0.04251111917989457 + "Value": 1.4, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -1989,18 +1989,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.171, - "Uncertainty": 0.009000000000000001 + "Cross section Ratio [-]": { + "Value": 1.413, + "Uncertainty": 0.026 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.524e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.520e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5238960166741713, - "Uncertainty": 0.042177458155728965 + "Value": 1.52, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2010,18 +2010,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.136, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 1.315, + "Uncertainty": 0.027 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.650e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.650e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6498917365448824, - "Uncertainty": 0.04181489080855449 + "Value": 1.65, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2031,18 +2031,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.076, - "Uncertainty": 0.01 + "Cross section Ratio [-]": { + "Value": 0.859, + "Uncertainty": 0.017 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.733e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.730e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7332659858757042, - "Uncertainty": 0.04155724207412975 + "Value": 1.73, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2052,18 +2052,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.017, - "Uncertainty": 0.011000000000000001 + "Cross section Ratio [-]": { + "Value": 0.967, + "Uncertainty": 0.021 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.816e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.820e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.8161122655967035, - "Uncertainty": 0.04128693460119519 + "Value": 1.82, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2073,18 +2073,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.068, - "Uncertainty": 0.017 + "Cross section Ratio [-]": { + "Value": 0.873, + "Uncertainty": 0.03 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.898e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.900e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.8984053399285274, - "Uncertainty": 0.04100405072802559 + "Value": 1.9, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2094,18 +2094,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.171, - "Uncertainty": 0.026000000000000002 + "Cross section Ratio [-]": { + "Value": 0.71, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=1.980e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.980e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.9801201416035437, - "Uncertainty": 0.04070867662378906 + "Value": 1.98, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2115,18 +2115,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.195, - "Uncertainty": 0.031000000000000003 + "Cross section Ratio [-]": { + "Value": 0.67, + "Uncertainty": 0.04 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.061e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.060e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.061231779501573, - "Uncertainty": 0.040400902262299136 + "Value": 2.06, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2136,18 +2136,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.47100000000000003, - "Uncertainty": 0.021 + "Cross section Ratio [-]": { + "Value": 2.78, + "Uncertainty": 0.15 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.182e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.180e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.1817143089415763, - "Uncertainty": 0.03991619634397461 + "Value": 2.18, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2157,18 +2157,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.361, - "Uncertainty": 0.015 + "Cross section Ratio [-]": { + "Value": 2.13, + "Uncertainty": 0.07 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.301e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.300e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.300701600373293, - "Uncertainty": 0.03940413385853442 + "Value": 2.3, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2178,18 +2178,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.27899999999999997, - "Uncertainty": 0.024 + "Cross section Ratio [-]": { + "Value": 1.77, + "Uncertainty": 0.09 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.418e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.420e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.418112105850723, - "Uncertainty": 0.03886506574802798 + "Value": 2.42, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2199,18 +2199,18 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": 0.184, - "Uncertainty": 0.042 + "Cross section Ratio [-]": { + "Value": 0.69, + "Uncertainty": 0.06 } }, - "frosch_electron_1968_electron_cross_section_ratio_Ca40_Ca48_q=2.534e+00": { + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.530e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.5338653580781973, - "Uncertainty": 0.0382993614628112 + "Value": 2.53, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -2220,9 +2220,9 @@ }, "Nuclide_A": "Ca40", "Nuclide_B": "Ca48", - "Cross section Ratio [fm^2/sr]": { - "Value": -0.11699999999999999, - "Uncertainty": 0.052000000000000005 + "Cross section Ratio [-]": { + "Value": 1.27, + "Uncertainty": 0.13 } } } diff --git a/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section.json b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section.json index da98234..fa50b3f 100644 --- a/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section.json +++ b/radbase/compilation/frosch_electron_1968/Electron Scattering Cross Section.json @@ -1,11 +1,11 @@ { - "frosch_electron_1968_electron_cross_section_Ca40_q=6.984e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=6.980e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.6984279472969682, - "Uncertainty": 0.021255559589947286 + "Value": 0.698, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -15,18 +15,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 63400.0, - "Uncertainty": 4500.0 + "Value": 6.3, + "Uncertainty": 0.5 }, "Notes": "Angular acceptance: 0.30" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=7.619e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=7.620e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.7619480083370856, - "Uncertainty": 0.021088729077864483 + "Value": 0.762, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -36,18 +36,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 27700.0, - "Uncertainty": 2000.0 + "Value": 2.77, + "Uncertainty": 0.2 }, "Notes": "Angular acceptance: 0.30" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=8.145e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=8.140e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.81448432585086, - "Uncertainty": 0.020938657891025794 + "Value": 0.814, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -57,18 +57,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 14000.0, - "Uncertainty": 1000.0 + "Value": 1.4, + "Uncertainty": 0.1 }, "Notes": "Angular acceptance: 0.30" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=8.666e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=8.670e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.8666329929378521, - "Uncertainty": 0.020778621037064876 + "Value": 0.867, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -78,18 +78,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 5890.0, - "Uncertainty": 350.0 + "Value": 0.589, + "Uncertainty": 0.035 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=9.081e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=9.080e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9080561327983517, - "Uncertainty": 0.020643467300597594 + "Value": 0.908, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -99,18 +99,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 3250.0, - "Uncertainty": 300.0 + "Value": 0.325, + "Uncertainty": 0.03 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=9.492e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=9.490e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9492026699642637, - "Uncertainty": 0.020502025364012796 + "Value": 0.949, + "Uncertainty": 0.021 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -120,18 +120,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 1610.0000000000002, - "Uncertainty": 100.0 + "Value": 0.161, + "Uncertainty": 0.01 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=9.901e-01": { + "frosch_electron_1968_electroncrosssection_Ca40_q=9.900e-01": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 0.9900600708017718, - "Uncertainty": 0.02035433831189453 + "Value": 0.99, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -141,18 +141,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 795.0, - "Uncertainty": 80.0 + "Value": 0.08, + "Uncertainty": 0.008 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.010e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.010e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.010376452315617, - "Uncertainty": 0.020278166851979997 + "Value": 1.01, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -162,18 +162,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 532.0, - "Uncertainty": 50.0 + "Value": 0.053, + "Uncertainty": 0.005 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.031e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.031e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0306158897507864, - "Uncertainty": 0.020200451131149568 + "Value": 1.031, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -183,18 +183,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 346.0, - "Uncertainty": 25.0 + "Value": 0.0346, + "Uncertainty": 0.0025 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.051e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.051e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0507768417957601, - "Uncertainty": 0.020121197067756273 + "Value": 1.051, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -204,18 +204,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 240.0, - "Uncertainty": 25.0 + "Value": 0.024, + "Uncertainty": 0.0025 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.071e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.071e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0708577731159827, - "Uncertainty": 0.02004041069730389 + "Value": 1.071, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -225,18 +225,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 162.0, - "Uncertainty": 15.0 + "Value": 0.0162, + "Uncertainty": 0.0015 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.091e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.091e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.0908571544707881, - "Uncertainty": 0.019958098171987303 + "Value": 1.091, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -246,18 +246,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 119.0, - "Uncertainty": 10.0 + "Value": 0.0119, + "Uncertainty": 0.001 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.111e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.111e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1107734628298558, - "Uncertainty": 0.019874265760223997 + "Value": 1.111, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -267,18 +267,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 82.69999999999999, - "Uncertainty": 4.0 + "Value": 0.0083, + "Uncertainty": 0.0004 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.150e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.150e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1503508001866465, - "Uncertainty": 0.01970206692926721 + "Value": 1.15, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -288,18 +288,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 53.800000000000004, - "Uncertainty": 4.0 + "Value": 0.0054, + "Uncertainty": 0.0004 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.170e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.170e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1700088152169004, - "Uncertainty": 0.019613713623681386 + "Value": 1.17, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -309,18 +309,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 47.1, - "Uncertainty": 5.0 + "Value": 0.0047, + "Uncertainty": 0.0005 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.190e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.190e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.1895777295460024, - "Uncertainty": 0.01952386665786555 + "Value": 1.19, + "Uncertainty": 0.02 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -330,18 +330,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 43.2, - "Uncertainty": 3.0 + "Value": 0.00432, + "Uncertainty": 0.0003 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.228e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.228e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2284423020052397, - "Uncertainty": 0.01933971922754796 + "Value": 1.228, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -351,18 +351,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 45.0, - "Uncertainty": 4.5 + "Value": 0.0045, + "Uncertainty": 0.0005 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.267e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.267e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.2669326790390987, - "Uncertainty": 0.0191496807314056 + "Value": 1.267, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -372,18 +372,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 48.2, - "Uncertainty": 3.0 + "Value": 0.00482, + "Uncertainty": 0.0003 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.343e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.343e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3427440662188048, - "Uncertainty": 0.01875216386875662 + "Value": 1.343, + "Uncertainty": 0.019 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -393,18 +393,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 45.4, - "Uncertainty": 3.0 + "Value": 0.00454, + "Uncertainty": 0.0003 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.417e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.417e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.416919526587691, - "Uncertainty": 0.01833180038298297 + "Value": 1.417, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -414,18 +414,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 32.400000000000006, - "Uncertainty": 2.5 + "Value": 0.00324, + "Uncertainty": 0.00025 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.489e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.489e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.4893686887731512, - "Uncertainty": 0.01788910242224003 + "Value": 1.489, + "Uncertainty": 0.018 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -435,18 +435,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 21.099999999999998, - "Uncertainty": 1.5 + "Value": 0.00211, + "Uncertainty": 0.00015 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.560e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.560e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5600032846310004, - "Uncertainty": 0.01742460934580058 + "Value": 1.56, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -456,18 +456,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 11.799999999999999, - "Uncertainty": 1.0 + "Value": 0.00118, + "Uncertainty": 0.0001 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.629e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.629e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6287372567866116, - "Uncertainty": 0.016938887066928577 + "Value": 1.629, + "Uncertainty": 0.017 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -477,18 +477,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 6.12, - "Uncertainty": 0.4 + "Value": 0.00061, + "Uncertainty": 4e-05 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.712e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.712e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.711854623334179, - "Uncertainty": 0.01630278459352114 + "Value": 1.712, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -498,18 +498,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 2.23, - "Uncertainty": 0.15 + "Value": 0.000223, + "Uncertainty": 1.5e-05 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.792e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.792e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7917133773107732, - "Uncertainty": 0.01563564884305023 + "Value": 1.792, + "Uncertainty": 0.016 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -519,18 +519,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.65, - "Uncertainty": 0.045000000000000005 + "Value": 6.500000000000001e-05, + "Uncertainty": 4.000000000000001e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.868e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.868e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.868161503039325, - "Uncertainty": 0.014938749746334384 + "Value": 1.868, + "Uncertainty": 0.015 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -540,18 +540,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.14200000000000002, - "Uncertainty": 0.010000000000000002 + "Value": 1.4200000000000001e-05, + "Uncertainty": 1.0000000000000002e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.941e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.941e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.9410534771674826, - "Uncertainty": 0.014213413890413367 + "Value": 1.941, + "Uncertainty": 0.014 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -561,18 +561,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.027000000000000007, - "Uncertainty": 0.0034999999999999996 + "Value": 2.7e-06, + "Uncertainty": 3.5e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.010e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.010e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.0102505456795847, - "Uncertainty": 0.013461021993314311 + "Value": 2.01, + "Uncertainty": 0.013 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -582,18 +582,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.0213, - "Uncertainty": 0.0025 + "Value": 2.13e-06, + "Uncertainty": 2.5e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.076e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.076e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.075620988022814, - "Uncertainty": 0.012683006275776504 + "Value": 2.076, + "Uncertainty": 0.013 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -603,18 +603,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.0392, - "Uncertainty": 0.0045000000000000005 + "Value": 3.9e-06, + "Uncertainty": 5e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.137e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.137e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.1370403678447563, - "Uncertainty": 0.011880847734937807 + "Value": 2.137, + "Uncertainty": 0.012 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -624,18 +624,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.0313, - "Uncertainty": 0.0055000000000000005 + "Value": 3.1e-06, + "Uncertainty": 6e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.248e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.248e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.247566022430375, - "Uncertainty": 0.010210253051446426 + "Value": 2.248, + "Uncertainty": 0.01 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 250.0, "Uncertainty": null }, @@ -645,18 +645,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.0221, - "Uncertainty": 0.003 + "Value": 2.21e-06, + "Uncertainty": 3e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.397e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.400e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.3968558945939364, - "Uncertainty": 0.04251111917989457 + "Value": 1.4, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -666,18 +666,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 168.0, - "Uncertainty": 12.0 + "Value": 0.0168, + "Uncertainty": 0.0012 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.524e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.520e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.5238960166741713, - "Uncertainty": 0.042177458155728965 + "Value": 1.52, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -687,18 +687,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 84.00000000000001, - "Uncertainty": 6.0 + "Value": 0.0084, + "Uncertainty": 0.0006 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.650e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.650e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.6498917365448824, - "Uncertainty": 0.04181489080855449 + "Value": 1.65, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -708,18 +708,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 29.799999999999997, - "Uncertainty": 2.2 + "Value": 0.00298, + "Uncertainty": 0.00022 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.733e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.730e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.7332659858757042, - "Uncertainty": 0.04155724207412975 + "Value": 1.73, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -729,18 +729,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 12.6, - "Uncertainty": 0.8999999999999999 + "Value": 0.00126, + "Uncertainty": 9e-05 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.816e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.820e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.8161122655967035, - "Uncertainty": 0.04128693460119519 + "Value": 1.82, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -750,18 +750,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 4.35, - "Uncertainty": 0.44 + "Value": 0.00043, + "Uncertainty": 4e-05 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.898e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.900e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.8984053399285274, - "Uncertainty": 0.04100405072802559 + "Value": 1.9, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -771,18 +771,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.983, - "Uncertainty": 0.064 + "Value": 9.800000000000001e-05, + "Uncertainty": 6e-06 }, "Notes": "Angular acceptance: 0.90" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=1.980e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=1.980e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 1.9801201416035437, - "Uncertainty": 0.04070867662378906 + "Value": 1.98, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -792,18 +792,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.266, - "Uncertainty": 0.023000000000000003 + "Value": 2.6600000000000003e-05, + "Uncertainty": 2.3000000000000004e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.061e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.060e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.061231779501573, - "Uncertainty": 0.040400902262299136 + "Value": 2.06, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -813,18 +813,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.22100000000000003, - "Uncertainty": 0.016 + "Value": 2.2100000000000002e-05, + "Uncertainty": 1.6000000000000001e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.182e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.180e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.1817143089415763, - "Uncertainty": 0.03991619634397461 + "Value": 2.18, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -834,18 +834,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.35000000000000003, - "Uncertainty": 0.022000000000000002 + "Value": 3.5000000000000004e-05, + "Uncertainty": 2.2e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.301e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.300e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.300701600373293, - "Uncertainty": 0.03940413385853442 + "Value": 2.3, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -855,18 +855,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.298, - "Uncertainty": 0.026000000000000002 + "Value": 2.9800000000000003e-05, + "Uncertainty": 2.6e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.418e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.420e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.418112105850723, - "Uncertainty": 0.03886506574802798 + "Value": 2.42, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -876,18 +876,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.185, - "Uncertainty": 0.022000000000000002 + "Value": 1.8500000000000002e-05, + "Uncertainty": 2.2e-06 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.534e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.530e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.5338653580781973, - "Uncertainty": 0.0382993614628112 + "Value": 2.53, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -897,18 +897,18 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.07980000000000001, - "Uncertainty": 0.008 + "Value": 8e-06, + "Uncertainty": 8e-07 }, "Notes": "Angular acceptance: 1.80" }, - "frosch_electron_1968_electron_cross_section_Ca40_q=2.648e+00": { + "frosch_electron_1968_electroncrosssection_Ca40_q=2.650e+00": { "Reference": "frosch_electron_1968", "q [1/fm]": { - "Value": 2.6478820255586437, - "Uncertainty": 0.037707408708343604 + "Value": 2.65, + "Uncertainty": 0.04 }, - "Energy [MeV]": { + "E [MeV]": { "Value": 500.0, "Uncertainty": null }, @@ -918,8 +918,8 @@ }, "Nuclide": "Ca40", "Cross section [fm^2/sr]": { - "Value": 0.025800000000000003, - "Uncertainty": 0.0040999999999999995 + "Value": 2.6e-06, + "Uncertainty": 4e-07 }, "Notes": "Angular acceptance: 1.80" } diff --git a/radbase/compilation/frosch_electron_1968/frosch_1968_process.py b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py index 273e779..f1fcb6f 100644 --- a/radbase/compilation/frosch_electron_1968/frosch_1968_process.py +++ b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py @@ -48,13 +48,16 @@ def convert_value(quantity_str): by_quant_dfs.to_csv('./cross_sections.csv', index=False) interface = DataEntryInterface(start_interface=False) +csr_procs = electron_scattering_cross_section_ratio_template.proc_dict +cs_procs = electron_scattering_cross_section_template.proc_dict for i, row in by_quant_dfs.iterrows(): if row['Value'] is None: continue - cs_values: dict = {'Reference': 'frosch_electron_1968'} + cs_values = {} + cs_values |= cs_procs['Reference'].process_data('frosch_electron_1968') theta, nrg = row['theta'], row['Energy [MeV]'] theta = ufloat(theta, 1) @@ -62,43 +65,36 @@ def convert_value(quantity_str): p_i = nrg_j / c # Ultra-relativistic q = 2 * p_i / hbar * sin(theta / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 - cs_values['q [1/fm]'] = {'Value': q.n, - 'Uncertainty': q.s} + cs_values |= cs_procs['q [1/fm]'].process_data(str(q)) - cs_values['Energy [MeV]'] = {'Value': nrg, - 'Uncertainty': None} - cs_values['theta [deg]'] = {'Value': theta.n, - 'Uncertainty': theta.s} + cs_values |= cs_procs['Energy [MeV]'].process_data(str(nrg)) + cs_values |= cs_procs['theta [deg]'].process_data(str(theta)) if 'D' in row['Quantity']: - cs_values['Nuclide_A'] = row['Quantity'][2:6] - cs_values['Nuclide_B'] = row['Quantity'][7:11] - cs_values['q [1/fm]'] = {'Value': q.n, - 'Uncertainty': q.s} + cs_values |= csr_procs['Nuclide A'].process_data(row['Quantity'][2:6]) + cs_values |= csr_procs['Nuclide B'].process_data(row['Quantity'][7:11]) + cs_values |= csr_procs['q [1/fm]'].process_data(str(q)) dratio = row['Value'] dratio, angular_acceptance = angle_acceptance(dratio) dratio = convert_value(dratio) / 100 # convert from percent ratio = (1 - dratio) / (1 + dratio) - cs_values['Cross section Ratio [fm^2/sr]'] = {'Value': dratio.n, - 'Uncertainty': dratio.s} + cs_values |= csr_procs['Cross section ratio (A/B) [-]'].process_data(str(ratio)) interface.save_data(electron_scattering_cross_section_ratio_template, cs_values, replacement_strategy='AlwaysReplace') - else: - cs_values['Nuclide'] = row['Quantity'] + cs_values |= cs_procs['Nuclide'].process_data(row['Quantity']) cs = row['Value'] cs, angular_acceptance = angle_acceptance(cs) cs = convert_value(cs) - cs *= 100 # microbarn to fm^2 conversion - cs_values['Cross section [fm^2/sr]'] = {'Value': cs.n, - 'Uncertainty': cs.s} + cs /= 100 # microbarn to fm^2 conversion + cs_values |= cs_procs['Cross section [fm^2/sr]'].process_data(str(cs)) - cs_values['Notes'] = (f'Angular acceptance: {angular_acceptance:0.2f}') + cs_values |= cs_procs['Notes'].process_data(f'Angular acceptance: {angular_acceptance:0.2f}') interface.save_data(electron_scattering_cross_section_template, cs_values, replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/heisenberg_electron_1972/Electron Scattering Cross Section Ratio.json b/radbase/compilation/heisenberg_electron_1972/Electron Scattering Cross Section Ratio.json new file mode 100644 index 0000000..fef5f5c --- /dev/null +++ b/radbase/compilation/heisenberg_electron_1972/Electron Scattering Cross Section Ratio.json @@ -0,0 +1,2354 @@ +{ + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=5.532e-01": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 32.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 0.5531549342591987, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 198.0, + "Uncertainty": null + }, + "Nuclide_A": "Ti46", + "Nuclide_B": "Ti48", + "Cross section Ratio [-]": { + "Value": 0.993, + "Uncertainty": 0.018 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=6.864e-01": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 40.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 0.6863733304067787, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 198.0, + "Uncertainty": null + }, + "Nuclide_A": "Ti46", + "Nuclide_B": "Ti48", + "Cross section Ratio [-]": { + "Value": 0.991, + "Uncertainty": 0.02 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=7.680e-01": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 45.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 0.7679772875652465, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 198.0, + "Uncertainty": null + }, + "Nuclide_A": "Ti46", + "Nuclide_B": "Ti48", + "Cross section Ratio [-]": { + "Value": 0.994, + "Uncertainty": 0.028 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.481e-01": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 50.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 0.8481193563078583, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 198.0, + "Uncertainty": null + }, + "Nuclide_A": "Ti46", + "Nuclide_B": "Ti48", + "Cross section Ratio [-]": { + "Value": 0.987, + "Uncertainty": 0.022 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.797e-01": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 52.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 0.8797325825612455, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 198.0, + "Uncertainty": null + }, + "Nuclide_A": "Ti46", + "Nuclide_B": "Ti48", + "Cross section Ratio [-]": { + "Value": 0.966, + "Uncertainty": 0.022 + } + }, + 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"Uncertainty": 0.03 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.137e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 44.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.137144798617188, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.18, + "Uncertainty": 0.05 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.186e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 46.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.1860919648205228, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.22, + "Uncertainty": 0.05 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.235e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 48.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.2346778359214423, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.22, + "Uncertainty": 0.04 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.283e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 50.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.2828876121929476, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.141, + "Uncertainty": 0.023 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.331e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 52.0, + "Uncertainty": null + }, + "q 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"Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.13, + "Uncertainty": 0.05 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.472e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 58.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.4716738778022775, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.134, + "Uncertainty": 0.021 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.518e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 60.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.5177853494888405, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.2, + "Uncertainty": 0.06 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.563e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 62.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.5634344890548324, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.19, + "Uncertainty": 0.05 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.609e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 64.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.6086073913301284, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.13, + "Uncertainty": 0.023 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.653e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 66.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.6532902962110956, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.19, + "Uncertainty": 0.06 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.697e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 68.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.6974695928520542, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.19, + "Uncertainty": 0.05 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.741e+00": { + "Reference": 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"Value": 1.8268520504849326, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.09, + "Uncertainty": 0.07 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.869e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 76.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.8688839349879387, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.46, + "Uncertainty": 0.12 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.910e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 78.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.9103465393400627, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.76, + "Uncertainty": 0.14 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.951e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 80.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 1.9512272336303609, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.22, + "Uncertainty": 0.09 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.031e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 84.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.0311932624521187, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.46, + "Uncertainty": 0.1 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.070e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 86.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.0702542385565508, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.24, + "Uncertainty": 0.08 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.146e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 90.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.1464726260183062, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.31, + "Uncertainty": 0.17 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.220e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 94.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.2200758672240197, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.43, + "Uncertainty": 0.09 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.291e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 98.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.2909742879619928, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.4, + "Uncertainty": 0.14 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.359e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 102.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.3590815094276194, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.13, + "Uncertainty": 0.13 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.424e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 106.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.424314553462658, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.13, + "Uncertainty": 0.15 + } + }, + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.487e+00": { + "Reference": "heisenberg_electron_1972", + "theta [deg]": { + "Value": 110.0, + "Uncertainty": null + }, + "q [1/fm]": { + "Value": 2.4865939436513314, + "Uncertainty": null + }, + "E [MeV]": { + "Value": 299.5, + "Uncertainty": null + }, + "Nuclide_A": "Ti48", + "Nuclide_B": "Ti50", + "Cross section Ratio [-]": { + "Value": 1.54, + "Uncertainty": 0.27 + } + } +} diff --git a/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_198MeV.csv b/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_198MeV.csv new file mode 100644 index 0000000..37ca96a --- /dev/null +++ b/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_198MeV.csv @@ -0,0 +1,28 @@ +theta,D(Ti46-Ti48),D(Ti48-Ti50) +32,0.33±0.92,1.36±0.92 +40,0.44±1.00,1.26±1.00 +45,0.32±1.40,-0.32±1.40 +50,0.63±1.10,0.32±1.10 +52,1.75±1.15,1.86±1.15 +54,1.35±1.25,3.45±1.25 +56,2.46±1.25,1.27±1.25 +58,5.20±1.35,0.17±1.35 +60,2.51±1.05,2.96±1.05 +62,2.02±1.10,0.16±1.10 +64,-0.76±0.65,-2.55±0.65 +66,-0.99±0.75,-2.51±0.75 +68,-4.57±1.00,-5.30±1.00 +70,-6.90±0.65,-4.33±0.65 +72,-6.63±0.75,-4.72±0.65 +74,-7.23±0.71,-5.00±0.77 +76,-7.56±0.82,-5.81±0.79 +78,-7.50±0.75,-5.63±0.76 +80,-10.00±0.94,-5.91±0.98 +82,-8.30±0.86,-4.60±0.86 +84,-9.30±1.04,-5.56±1.11 +86,-8.80±0.86,-5.24±0.81 +90,-7.45±0.78,-6.22±0.80 +95,-6.20±0.84,-7.02±0.82 +100,-6.20±0.97,-7.35±0.95 +105,-7.58±1.29,-4.21±1.24 +110,...,-6.14±1.50 diff --git a/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_299p5MeV.csv b/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_299p5MeV.csv new file mode 100644 index 0000000..ecb015a --- /dev/null +++ b/radbase/compilation/heisenberg_electron_1972/cross_section_ratios_299p5MeV.csv @@ -0,0 +1,34 @@ +theta,D(Ti46-Ti48),D(Ti48-Ti50) +38,4.2±1.5,-3.8±1.6 +40,2.9±2.4,1.2±2.5 +42,-1.9±1.4,-3.0±1.4 +44,-5.3±2.4,-8.3±2.2 +46,-4.2±2.1,-9.8±1.9 +48,-9.3±1.8,-9.8±1.8 +50,-8.9±1.1,-6.6±1.0 +52,-3.8±1.8,-11.0±1.8 +54,-8.6±1.8,-5.3±1.9 +56,-9.4±2.1,-6.0±2.0 +58,-6.7±0.9,-6.3±0.9 +60,-3.1±2.6,-8.9±2.3 +62,-2.7±2.1,-8.8±2.0 +64,-7.7±3.1,-8.9±2.9 +64,-7.9±1.1,-6.1±1.0 +66,2.1±2.7,-8.5±2.6 +68,-4.0±2.1,-8.7±1.9 +70,-0.4±2.2,-6.2±2.1 +72,-3.2±3.3,-12.1±3.0 +74,-25.0±4.2,-4.4±3.3 +76,-19.7±8.6,-11.3±7.3 +76,-3.7±4.7,-18.6±4.1 +78,-4.8±4.3,-27.5±3.6 +80,-36.3±9.3,-17.9±6.3 +80,-24.7±4.6,-10.0±3.8 +84,-11.3±3.6,-18.7±3.2 +86,-26.8±3.7,-10.6±3.2 +90,-13.2±6.5,-13.6±6.4 +94,-19.7±3.3,-17.7±3.2 +98,-5.9±5.1,-16.7±4.8 +102,-16.2±5.9,-6.1±5.6 +106,-22.6±7.7,-6.3±6.6 +110,...,-21.2±8.5 diff --git a/radbase/compilation/heisenberg_electron_1972/heisenberg_1972_process.py b/radbase/compilation/heisenberg_electron_1972/heisenberg_1972_process.py new file mode 100644 index 0000000..cd6c81d --- /dev/null +++ b/radbase/compilation/heisenberg_electron_1972/heisenberg_1972_process.py @@ -0,0 +1,69 @@ +import re + +import pandas as pd +from scipy.constants import c, electron_volt, hbar, pi +from uncertainties import ufloat, ufloat_fromstr +from uncertainties.umath import sin + +from radbase.data_entry import ( + DataEntryInterface, electron_scattering_cross_section_ratio_template) + + +def angle_acceptance(quantity_str): + angle_acceptances = {'ᵃ': 0.9, 'ᵇ': 0.3, 'ᶜ': 0.36, 'ᵈ': 0.2} + if quantity_str[-1] in angle_acceptances: + return quantity_str[:-1], angle_acceptances[quantity_str[-1]] + else: + return quantity_str, 1.8 + + +def convert_value(quantity_str): + quantity_str = quantity_str.replace('−', '-') + if len(matches := re.findall(r'\([^)^(]*\)', quantity_str)) == 2: + value, exponent = matches + value = ufloat_fromstr(value[1:-1]) * 10 ** int(exponent[1:-1]) + else: + value = ufloat_fromstr(quantity_str) + return value + + +df198MeV = pd.read_csv('./cross_section_ratios_198MeV.csv') +df299p5MeV = pd.read_csv('./cross_section_ratios_299p5MeV.csv') + +interface = DataEntryInterface(start_interface=False) +csr_procs = electron_scattering_cross_section_ratio_template.proc_dict + +for (df, nrg) in [(df198MeV, 198), (df299p5MeV, 299.5)]: + for col in df.columns: + if col == 'theta': + continue + + for i, row in df.iterrows(): + + if row[col] is None or row[col] in ['', '...']: + continue + + csr_values = {} + csr_values |= csr_procs['Reference'].process_data('heisenberg_electron_1972') + + theta = row['theta'] + csr_values |= csr_procs['theta [deg]'].process_data(theta) + + nrg_j = nrg * electron_volt * 10 ** 6 + p_i = nrg_j / c # Ultra-relativistic + q = 2 * p_i / hbar * sin(float(theta) / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 + csr_values |= csr_procs['q [1/fm]'].process_data(str(q)) + + csr_values |= csr_procs['Energy [MeV]'].process_data(str(nrg)) + + csr_values |= csr_procs['Nuclide A'].process_data(col[2:6]) + csr_values |= csr_procs['Nuclide B'].process_data(col[7:11]) + + dratio = row[col] + dratio = convert_value(dratio) / 100 # convert from percent + ratio = (1 - dratio) / (1 + dratio) + + csr_values |= csr_procs['Cross section ratio (A/B) [-]'].process_data(str(ratio)) + + interface.save_data(electron_scattering_cross_section_ratio_template, csr_values, + replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json b/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json index affc936..bdbda9b 100644 --- a/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json +++ b/radbase/compilation/lightbody_elastic_1983/Electron Scattering Cross Section Ratio.json @@ -1,1512 +1,1512 @@ { - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=1.520e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.520e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.15203192148469183, - "Uncertainty": 0.0022979616877686717 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 30, + "E [MeV]": { + "Value": 30.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9977, "Uncertainty": 0.0053 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=1.520e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.520e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.15203192148469183, - "Uncertainty": 0.0022979616877686717 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 30, + "E [MeV]": { + "Value": 30.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0019, "Uncertainty": 0.0058 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=1.520e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.520e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.15203192148469183, - "Uncertainty": 0.0022979616877686717 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 30, + "E [MeV]": { + "Value": 30.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9995, "Uncertainty": 0.0031 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=1.774e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.774e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.17737057506547382, - "Uncertainty": 0.0026809553023967843 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 35, + "E [MeV]": { + "Value": 35.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0108, "Uncertainty": 0.0057 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=1.774e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.774e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.17737057506547382, - "Uncertainty": 0.0026809553023967843 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 35, + "E [MeV]": { + "Value": 35.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9896, "Uncertainty": 0.0055 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=1.774e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.774e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.17737057506547382, - "Uncertainty": 0.0026809553023967843 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 35, + "E [MeV]": { + "Value": 35.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0003, "Uncertainty": 0.003 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.027e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.027e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2027092286462558, - "Uncertainty": 0.003063948917024896 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 40, + "E [MeV]": { + "Value": 40.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0046, "Uncertainty": 0.0088 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.027e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.027e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2027092286462558, - "Uncertainty": 0.003063948917024896 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 40, + "E [MeV]": { + "Value": 40.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9903, "Uncertainty": 0.0059 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=2.027e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.027e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2027092286462558, - "Uncertainty": 0.003063948917024896 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 40, + "E [MeV]": { + "Value": 40.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9949, "Uncertainty": 0.0054 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.280e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.280e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.22804788222703773, - "Uncertainty": 0.0034469425316530074 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 45, + "E [MeV]": { + "Value": 45.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0025, "Uncertainty": 0.0061 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.280e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.280e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.22804788222703773, - "Uncertainty": 0.0034469425316530074 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 45, + "E [MeV]": { + "Value": 45.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9919, "Uncertainty": 0.0058 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=2.280e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.280e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.22804788222703773, - "Uncertainty": 0.0034469425316530074 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 45, + "E [MeV]": { + "Value": 45.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9944, "Uncertainty": 0.0035 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.534e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.534e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2533865358078198, - "Uncertainty": 0.00382993614628112 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 50, + "E [MeV]": { + "Value": 50.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0091, "Uncertainty": 0.0067 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.534e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.534e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2533865358078198, - "Uncertainty": 0.00382993614628112 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 50, + "E [MeV]": { + "Value": 50.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9885, "Uncertainty": 0.0056 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=2.534e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.534e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.2533865358078198, - "Uncertainty": 0.00382993614628112 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 50, + "E [MeV]": { + "Value": 50.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9975, "Uncertainty": 0.004 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=2.787e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.787e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.27872518938860175, - "Uncertainty": 0.004212929760909232 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 55, + "E [MeV]": { + "Value": 55.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0028, "Uncertainty": 0.0064 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=2.787e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.787e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.27872518938860175, - "Uncertainty": 0.004212929760909232 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 55, + "E [MeV]": { + "Value": 55.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9888, "Uncertainty": 0.007 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=2.787e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.787e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.27872518938860175, - "Uncertainty": 0.004212929760909232 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 55, + "E [MeV]": { + "Value": 55.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9916, "Uncertainty": 0.0044 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=3.041e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.041e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.30406384296938366, - "Uncertainty": 0.004595923375537343 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 60, + "E [MeV]": { + "Value": 60.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 1.0155, "Uncertainty": 0.0075 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=3.041e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.041e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.30406384296938366, - "Uncertainty": 0.004595923375537343 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 60, + "E [MeV]": { + "Value": 60.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.98, "Uncertainty": 0.0073 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=3.041e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.041e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.30406384296938366, - "Uncertainty": 0.004595923375537343 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 60, + "E [MeV]": { + "Value": 60.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9952, "Uncertainty": 0.0044 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=3.294e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.294e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.3294024965501656, - "Uncertainty": 0.0049789169901654565 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 65, + "E [MeV]": { + "Value": 65.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr52", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9993, "Uncertainty": 0.0068 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr52_q=3.294e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.294e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.3294024965501656, - "Uncertainty": 0.0049789169901654565 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 65, + "E [MeV]": { + "Value": 65.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr52", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.988, "Uncertainty": 0.0063 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr54_Cr50_q=3.294e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.294e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.3294024965501656, - "Uncertainty": 0.0049789169901654565 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 65, + "E [MeV]": { + "Value": 65.0, "Uncertainty": null }, "theta [deg]": { "Value": 60.0, - "Uncertainty": 1.0 + "Uncertainty": null }, "Nuclide_A": "Cr54", "Nuclide_B": "Cr50", - "Cross section Ratio (A/B) [fm^2/sr]": { + "Cross section Ratio [-]": { "Value": 0.9873, "Uncertainty": 0.0039 } }, - "lightbody_elastic_1983_electron_cross_section_ratio_Cr52_Cr50_q=3.547e-01": { + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.547e-01": { "Reference": "lightbody_elastic_1983", "q [1/fm]": { "Value": 0.35474115013094765, - "Uncertainty": 0.005361910604793569 + "Uncertainty": null }, - "Energy [MeV]": { - "Value": 70, + "E [MeV]": { 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+41,200,0.3187(69)+0, +45,200,0.1188(28)+0, +50,200,0.2809(64)-1,±0.4,±1.15 +55,200,0.608(14)-2, +60,200,0.1588(39)-2,±0.4,±4.0 +65,200,0.1160(32)-2,±0.9,±2.9 +70,200,0.1177(31)-2, +75,200,0.985(29)-3, +80,200,0.654(20)-3, +85.06,200,0.442(14)-3, +90,200,0.2076(69)-3, +95,200,0.1133(44)-3, +38,200,0.666(16)+0,±0.3,±0.3 +35,401.6,0.466(13)-2,±0.9,±2.7 +40,401.6,0.2302(94)-2, +47.5,401.6,0.1784(70)-3,±1.0,±4.0 +60,401.6,0.948(47)-5,±0.9,±2.7 +62.5,401.6,0.880(34)-5, +67.5,401.6,0.468(19)-5,±1.0,±4.0 +72.5,401.6,0.1188(71)-5, +77.5,401.6,0.228(23)-6, +35,398.2,0.540(21)-2,±0.9,±2.7 +37.5,398.2,0.384(15)-2,±1.08,±4.0 +40,398.2,0.2395(94)-2, +42.5,398.2,0.1248(49)-2, +47.5,398.2,0.2000(79)-3, +50,398.2,0.521(21)-4, +52.5,398.2,0.1154(43)-5, +55,398.2,0.643(26)-5, +57.5,398.2,0.912(36)-5, +60,398.2,0.1084(43)-4, +62.5,398.2,0.976(39)-5, +65,398.2,0.726(30)-5, +70,398.2,0.2439(96)-5, +75,398.2,0.720(75)-6, +80,398.2,0.72(12)-7, diff --git a/radbase/compilation/lightbody_elastic_1983/cross_section_Cr54.csv b/radbase/compilation/lightbody_elastic_1983/cross_section_Cr54.csv new file mode 100644 index 0000000..cf55308 --- /dev/null +++ b/radbase/compilation/lightbody_elastic_1983/cross_section_Cr54.csv @@ -0,0 +1,62 @@ +Energy [MeV],theta,cross_section,theta_acceptance,phi_acceptance +30,60,0.4268(30)+2,±0.0,±0.0 +35,60,0.2965(23)+2,, +40,60,0.2154(16)+2,, +45,60,0.1599(13)+2,, +50,60,0.1205(09)+2,, +55,60,0.9193(76)+1,, +60,60,0.7055(57)+1,, +65,60,0.5507(44)+1,, +70,60,0.4296(35)+1,, +75,60,0.3337(25)+1,, +80,60,0.2666(20)+1,, +85,60,0.2082(16)+1,, +30,120,0.1297(09)+1,, +35,120,0.8156(72)+0,, +40,120,0.5215(39)+0,, +45,120,0.3428(29)+0,, +50,120,0.2160(19)+0,, +55,120,0.1404(14)+0,, +60,120,0.8759(82)-1,, +65,120,0.5462(46)-1,, +70,120,0.3286(32)-1,, +75,120,0.1960(20)-1,, +80,120,0.1100(09)-1,, +85,120,0.5968(50)-2,, +35,200,0.1275(28)+1,±0.3,±0.3 +38.05,200,0.606(15)+0,, +41,200,0.2981(72)+0,, +45,200,0.1040(26)+0,, +50,200,0.2524(64)-1,±0.4,±1.15 +55,200,0.523(13)-2,, +60,200,0.1458(37)-2,±0.4,±4.0 +65,200,0.1125(33)-2,±0.9,±2.9 +70,200,0.1078(31)-2,, +75,200,0.933(29)-3,, +80,200,0.602(18)-3,, +85.06,200,0.345(12)-3,, +90,200,0.1939(70)-3,, +95,200,0.856(34)-4,, +38,200,0.612(14)-4,±0.3,±0.3 +35,401.6,0.422(17)-2,±0.9,±2.7 +40,401.6,0.1991(83)-2,, +47.5,401.6,0.1413(59)-3,±1.0,±4.0 +60,401.6,0.866(36)-5,±0.9,±2.7 +62.4,401.6,0.670(28)-5,, +67.5,401.6,0.2699(96)-5,±1.0,±4.0 +72.5,401.6,0.708(52)-6,, +77.4,401.6,0.41(13)-7,, +35,398.2,0.487(20)-2,±0.9,±2.7 +37.5,398.2,0.338(13)-2,±1.08,±4.0 +40,398.2,0.2200(91)-2,, +42.5,398.2,0.1039(43)-2,, +47.5,398.2,0.1541(63)-3,, +52.5,398.2,0.895(37)-5,, +55,398.2,0.569(23)-5,, +57.5,398.2,0.750(31)-5,, +60,398.2,0.981(41)-5,, +62.5,398.2,0.700(29)-5,, +65,398.2,0.504(21)-5,, +70,398.2,0.1554(63)-5,, +75,398.2,0.360(38)-6,, +80,398.2,0.31(15)-7,, diff --git a/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py b/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py index 0df3f6b..6d750b7 100644 --- a/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py +++ b/radbase/compilation/lightbody_elastic_1983/lightbody_1983_process.py @@ -1,41 +1,78 @@ +import re + import pandas as pd from scipy.constants import c, electron_volt, hbar, pi from uncertainties import ufloat, ufloat_fromstr from uncertainties.umath import sin from radbase.data_entry import ( - DataEntryInterface, electron_scattering_cross_section_ratio_template) + DataEntryInterface, electron_scattering_cross_section_ratio_template, + electron_scattering_cross_section_template) interface = DataEntryInterface(start_interface=False) +csr_procs = electron_scattering_cross_section_ratio_template.proc_dict +cs_procs = electron_scattering_cross_section_template.proc_dict df = pd.read_csv('./cross_section_ratios.csv') for i, row in df.iterrows(): theta, nrg = row['theta'], row['Energy [MeV]'] - theta = ufloat(theta, 1) nrg_j = nrg * electron_volt * 10 ** 6 p_i = nrg_j / c # Ultra-relativistic q = 2 * p_i / hbar * sin(theta / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 for col in ['Cr52/Cr50', 'Cr54/Cr52', 'Cr54/Cr50']: - cs_values: dict = {'Reference': 'lightbody_elastic_1983'} + csr_values = {} + + csr_values |= csr_procs['Reference'].process_data('lightbody_elastic_1983') + csr_values |= csr_procs['q [1/fm]'].process_data(str(q)) + csr_values |= csr_procs['Energy [MeV]'].process_data(str(nrg)) + csr_values |= csr_procs['theta [deg]'].process_data(row['theta']) + + csr_values |= csr_procs['Nuclide A'].process_data(col[:4]) + csr_values |= csr_procs['Nuclide B'].process_data(col[5:]) + + csr_values |= csr_procs['Cross section ratio (A/B) [-]'].process_data(row[col]) + + interface.save_data(electron_scattering_cross_section_ratio_template, csr_values, + replacement_strategy='AlwaysReplace') + + +def convert_value(quantity_str): + quantity_str = quantity_str.replace('−', '-') + if len(matches := re.findall(r'\([^)^(]*\)', quantity_str)) == 2: + value, exponent = matches + value = ufloat_fromstr(value[1:-1]) * 10 ** int(exponent[1:-1]) + else: + value = ufloat_fromstr(quantity_str[:-2]) * 10 ** int(quantity_str[-2:]) + return value + + +for nuclide, df in [('Cr50', pd.read_csv('./cross_section_Cr50.csv')), + ('Cr52', pd.read_csv('./cross_section_Cr52.csv')), + ('Cr54', pd.read_csv('./cross_section_Cr54.csv'))]: + + df.ffill(inplace=True) - cs_values['q [1/fm]'] = {'Value': q.n, - 'Uncertainty': q.s} + for i, row in df.iterrows(): - cs_values['Energy [MeV]'] = {'Value': nrg, - 'Uncertainty': None} - cs_values['theta [deg]'] = {'Value': theta.n, - 'Uncertainty': theta.s} + theta, nrg = row['theta'], row['Energy [MeV]'] + theta = ufloat(theta, 1) + nrg_j = nrg * electron_volt * 10 ** 6 + p_i = nrg_j / c # Ultra-relativistic + q = 2 * p_i / hbar * sin(theta / 2 * pi / 180) * 10 ** -15 # in units of fm^-1 - cs_values['Nuclide_A'] = col[:4] - cs_values['Nuclide_B'] = col[5:] + cs_values = {} - ratio = ufloat_fromstr(row[col]) + cs_values |= cs_procs['Reference'].process_data('lightbody_elastic_1983') + cs_values |= cs_procs['q [1/fm]'].process_data(str(q)) + cs_values |= cs_procs['Energy [MeV]'].process_data(str(nrg)) + cs_values |= cs_procs['theta [deg]'].process_data(row['theta']) + cs_values |= cs_procs['Nuclide'].process_data(nuclide) - cs_values['Cross section Ratio (A/B) [fm^2/sr]'] = {'Value': ratio.n, - 'Uncertainty': ratio.s} + cs = convert_value(row['cross_section']) * 10 # mb to fm^2 + cs_values |= cs_procs['Cross section [fm^2/sr]'].process_data(str(cs)) - interface.save_data(electron_scattering_cross_section_ratio_template, cs_values, + interface.save_data(electron_scattering_cross_section_template, cs_values, replacement_strategy='AlwaysReplace') diff --git a/radbase/compilation/references.json b/radbase/compilation/references.json index 4c21e58..0da1801 100644 --- a/radbase/compilation/references.json +++ b/radbase/compilation/references.json @@ -261,5 +261,103 @@ "pages": "533-548", "url": "https://link.aps.org/doi/10.1103/PhysRevC.23.533", "doi": "10.1103/PhysRevC.23.533" + }, + "heisenberg_electron_1972": { + "title": "Electron-Scattering Determination of Isotopic Differences in the Charge Distributions of Ti46, 48, 50", + "author": [ + "J. Heisenberg", + "R. Hofstadter", + "J. S. McCarthy", + "R. Herman", + "B. C. Clark", + "D. G. Ravenhall" + ], + "year": "1972", + "month": "July", + "journal": "Physical Review C", + "volume": "6", + "pages": "381-384", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.6.381", + "doi": "10.1103/PhysRevC.6.381" + }, + "tanaka_measurement_1984": { + "title": "Measurement and analysis of muonic x rays of 176,177, 178, 179, 180Hf", + "author": [ + "Y. Tanaka", + "R. M. Steffen", + "E. B. Shera", + "W. Reuter", + "M. V. Hoehn", + "J. D. Zumbro" + ], + "year": "1984", + "month": "July", + "journal": "Physical Review C", + "volume": "30", + "pages": "350-359", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.30.350", + "doi": "10.1103/PhysRevC.30.350" + }, + "lightbody_elastic_1983": { + "title": "Elastic and inelastic electron scattering from 50,52,54Cr", + "author": [ + "J. W. Lightbody,Jr", + "J. B. Bellicard", + "J. M. Cavedon", + "B. Frois", + "D. Goutte", + "M. Huet", + "Ph. Leconte", + "A. Nakada", + "Phan Xuan Ho", + "S. K. Platchkov", + "S. Turck-Chieze" + ], + "year": "1983", + "month": "January", + "journal": "Physical Review C", + "volume": "27", + "pages": "113-132", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.27.113", + "doi": "10.1103/PhysRevC.27.113" + }, + "frosch_electron_1968": { + "title": "Electron Scattering Studies of Calcium and Titanium Isotopes", + "author": [ + "R. F. Frosch", + "R. Hofstadter", + "J. S. McCarthy", + "G. K. N\u00f6ldeke", + "K. J. van OostraM", + "M. R. Yearian" + ], + "year": "1968", + "month": "October", + "journal": "Physical Review", + "volume": "174", + "pages": "1380-1399", + "url": "https://link.aps.org/doi/10.1103/PhysRev.174.1380", + "doi": "10.1103/PhysRev.174.1380" + }, + "schaller_nuclear_1985": { + "title": "Nuclear charge radii of the even sulphur isotopes 32S, 34S, and 36S and of 31P using muonic atoms", + "author": [ + "L. A. Schaller", + "D. A. Barandao", + "P. Bergem", + "M. Boschung", + "T. Q. Phan", + "G. Piller", + "A. Ruetschi", + "L. Schellenberg", + "H. Schneuwly" + ], + "year": "1985", + "month": "March", + "journal": "Physical Review C", + "volume": "31", + "pages": "1007-1011", + "url": "https://link.aps.org/doi/10.1103/PhysRevC.31.1007", + "doi": "10.1103/PhysRevC.31.1007" } } diff --git a/radbase/compilation/schaller_nuclear_1985/Muonic Transition Energy.json b/radbase/compilation/schaller_nuclear_1985/Muonic Transition Energy.json new file mode 100644 index 0000000..81e71d1 --- /dev/null +++ b/radbase/compilation/schaller_nuclear_1985/Muonic Transition Energy.json @@ -0,0 +1,15 @@ +{ + "schaller_nuclear_1985_muonic_P31_2p_1s": { + "Reference": "schaller_nuclear_1985", + "Nuclide": "P31", + "Transition": { + "Upper": "2p", + "Lower": "1s" + }, + "Energy [keV]": { + "Value": 456.806, + "Uncertainty": 0.012 + }, + "Notes": "Recoil corrected; #stat_unc #cal_unc #sys_unc" + } +} diff --git a/radbase/compilation/tanaka_measurement_1984/Muonic Transition Energy.json b/radbase/compilation/tanaka_measurement_1984/Muonic Transition Energy.json new file mode 100644 index 0000000..8f1caa0 --- /dev/null +++ b/radbase/compilation/tanaka_measurement_1984/Muonic Transition Energy.json @@ -0,0 +1,28 @@ +{ + "tanaka_measurement_1984_muonic_Hf176_(2+,2p3/2)1/2-_(2+,1s1/2)3/2+": { + "Reference": "tanaka_measurement_1984", + "Nuclide": "Hf176", + "Transition": { + "Upper": "(2+,2p3/2)1/2-", + "Lower": "(2+,1s1/2)3/2+" + }, + "Energy [keV]": { + "Value": 5214.21, + "Uncertainty": 0.73 + }, + "Notes": "#Stat_only" + }, + "tanaka_measurement_1984_muonic_Hf176_(0+,2p3/2)3/2-_(0+,1s1/2)1/2+": { + "Reference": "tanaka_measurement_1984", + "Nuclide": "Hf176", + "Transition": { + "Upper": "(0+,2p3/2)3/2-", + "Lower": "(0+,1s1/2)1/2+" + }, + "Energy [keV]": { + "Value": 5268.95, + "Uncertainty": 0.23 + }, + "Notes": "Blend of I=1/2+ and I=3/2+ for 0+,1s1/2 level. #Stat_only" + } +} diff --git a/radbase/compilation/test_test_1700/Muonic Barrett Moment.json b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json index 99c0fa2..5461d2d 100644 --- a/radbase/compilation/test_test_1700/Muonic Barrett Moment.json +++ b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json @@ -15,5 +15,2606 @@ "Nuclear Polarization Method": "Calculated", "Calculated Nuclear Polarization": [], "Notes": "" + }, + "test_test_1700_barrettmoment_P32_Pb208-2p1/2-1s1/2_Pb208-2p3/2-1s1/2_Pb208-2s1/2-2p3/2_2s1/2-2p1/2_Pb208-3d3/2-2p1/2_Pb208-3d3/2-2p3/2_Pb208-3d5/2-2p3/2_Pb208-3p1/2-2s1/2_Pb208-3p3/2-2s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3f7/2-3d5/2_3p1/2-2s1/2_3p3/2-2s1/2_4d3/2-3p1/2_4d3/2-3p3/2_4d5/2-3p3/2_4f5/2-3d3/2_4f5/2-3d5/2_5f5/2-3d3/2_5f5/2-3d5/2_5f7/2-3d5/2_NP-Calculated_NP-Fit_Ca40-q=1.010e+00_Ca40-q=1.031e+00_Ca40-q=1.051e+00_Ca40-q=1.071e+00_Ca40-q=1.091e+00_Ca40-q=1.111e+00_Ca40-q=1.150e+00_Ca40-q=1.170e+00_Ca40-q=1.190e+00_Ca40-q=1.228e+00_Ca40-q=1.267e+00_Ca40-q=1.343e+00_Ca40-q=1.400e+00_Ca40-q=1.417e+00_Ca40-q=1.489e+00_Ca40-q=1.520e+00_Ca40-q=1.560e+00_Ca40-q=1.629e+00_Ca40-q=1.650e+00_Ca40-q=1.712e+00_Ca40-q=1.730e+00_Ca40-q=1.792e+00_Ca40-q=1.820e+00_Ca40-q=1.868e+00_Ca40-q=1.900e+00_Ca40-q=1.941e+00_Ca40-q=1.980e+00_Ca40-q=2.010e+00_Ca40-q=2.060e+00_Ca40-q=2.076e+00_Ca40-q=2.137e+00_Ca40-q=2.180e+00_Ca40-q=2.248e+00_Ca40-q=2.300e+00_Ca40-q=2.420e+00_Ca40-q=2.530e+00_Ca40-q=2.650e+00_Ca40-q=6.980e-01_Ca40-q=7.620e-01_Ca40-q=8.140e-01_Ca40-q=8.670e-01_Ca40-q=9.080e-01_Ca40-q=9.490e-01_Ca40-q=9.900e-01_Ca42-q=1.031e+00_Ca42-q=1.071e+00_Ca42-q=1.111e+00_Ca42-q=1.150e+00_Ca42-q=1.190e+00_Ca42-q=1.267e+00_Ca42-q=1.343e+00_Ca42-q=1.417e+00_Ca42-q=1.489e+00_Ca42-q=1.560e+00_Ca42-q=1.629e+00_Ca42-q=1.695e+00_Ca42-q=6.980e-01_Ca42-q=7.830e-01_Ca42-q=8.670e-01_Ca42-q=9.490e-01_Ca44-q=1.031e+00_Ca44-q=1.071e+00_Ca44-q=1.111e+00_Ca44-q=1.150e+00_Ca44-q=1.190e+00_Ca44-q=1.267e+00_Ca44-q=1.343e+00_Ca44-q=1.417e+00_Ca44-q=1.489e+00_Ca44-q=1.560e+00_Ca44-q=1.629e+00_Ca44-q=1.712e+00_Ca44-q=1.792e+00_Ca44-q=6.980e-01_Ca44-q=7.620e-01_Ca44-q=8.140e-01_Ca44-q=8.670e-01_Ca44-q=9.080e-01_Ca44-q=9.490e-01_Ca44-q=9.900e-01_Ca48-q=1.010e+00_Ca48-q=1.031e+00_Ca48-q=1.051e+00_Ca48-q=1.071e+00_Ca48-q=1.091e+00_Ca48-q=1.111e+00_Ca48-q=1.131e+00_Ca48-q=1.150e+00_Ca48-q=1.170e+00_Ca48-q=1.190e+00_Ca48-q=1.228e+00_Ca48-q=1.267e+00_Ca48-q=1.305e+00_Ca48-q=1.343e+00_Ca48-q=1.400e+00_Ca48-q=1.417e+00_Ca48-q=1.489e+00_Ca48-q=1.520e+00_Ca48-q=1.560e+00_Ca48-q=1.629e+00_Ca48-q=1.650e+00_Ca48-q=1.712e+00_Ca48-q=1.730e+00_Ca48-q=1.792e+00_Ca48-q=1.820e+00_Ca48-q=1.868e+00_Ca48-q=1.900e+00_Ca48-q=1.941e+00_Ca48-q=1.980e+00_Ca48-q=2.010e+00_Ca48-q=2.060e+00_Ca48-q=2.076e+00_Ca48-q=2.137e+00_Ca48-q=2.180e+00_Ca48-q=2.248e+00_Ca48-q=2.300e+00_Ca48-q=2.420e+00_Ca48-q=2.530e+00_Ca48-q=6.980e-01_Ca48-q=7.620e-01_Ca48-q=8.140e-01_Ca48-q=8.670e-01_Ca48-q=9.080e-01_Ca48-q=9.490e-01_Ca48-q=9.900e-01_Ti48-q=1.031e+00_Ti48-q=1.071e+00_Ti48-q=1.111e+00_Ti48-q=1.150e+00_Ti48-q=1.190e+00_Ti48-q=1.228e+00_Ti48-q=1.267e+00_Ti48-q=1.305e+00_Ti48-q=1.343e+00_Ti48-q=1.380e+00_Ti48-q=1.417e+00_Ti48-q=1.453e+00_Ti48-q=1.489e+00_Ti48-q=1.525e+00_Ti48-q=1.560e+00_Ti48-q=1.629e+00_Ti48-q=1.712e+00_Ti48-q=1.792e+00_Ti48-q=6.980e-01_Ti48-q=7.620e-01_Ti48-q=8.140e-01_Ti48-q=8.670e-01_Ti48-q=9.080e-01_Ti48-q=9.490e-01_Ti48-q=9.900e-01_fermi-Hg198_fermi-Hg199_fermi-Hg200_fermi-Hg201_fermi-Hg202_fermi-Hg204_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_3d3/2-2p1/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_3d3/2-2p1/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_Hg199-1s1/2_Hg200-1s1/2_Hg201-1s1/2_Hg202-1s1/2_Hg204-1s1/2_Ti48-q=1.003e+00_Ti48-q=1.034e+00_Ti48-q=1.038e+00_Ti48-q=1.063e+00_Ti48-q=1.088e+00_Ti48-q=1.093e+00_Ti48-q=1.122e+00_Ti48-q=1.137e+00_Ti48-q=1.151e+00_Ti48-q=1.180e+00_Ti48-q=1.186e+00_Ti48-q=1.208e+00_Ti48-q=1.235e+00_Ti48-q=1.236e+00_Ti48-q=1.263e+00_Ti48-q=1.283e+00_Ti48-q=1.290e+00_Ti48-q=1.317e+00_Ti48-q=1.331e+00_Ti48-q=1.343e+00_Ti48-q=1.369e+00_Ti48-q=1.378e+00_Ti48-q=1.419e+00_Ti48-q=1.425e+00_Ti48-q=1.472e+00_Ti48-q=1.480e+00_Ti48-q=1.518e+00_Ti48-q=1.537e+00_Ti48-q=1.563e+00_Ti48-q=1.592e+00_Ti48-q=1.609e+00_Ti48-q=1.653e+00_Ti48-q=1.697e+00_Ti48-q=1.741e+00_Ti48-q=1.784e+00_Ti48-q=1.827e+00_Ti48-q=1.869e+00_Ti48-q=1.910e+00_Ti48-q=1.951e+00_Ti48-q=2.031e+00_Ti48-q=2.070e+00_Ti48-q=2.146e+00_Ti48-q=2.220e+00_Ti48-q=2.291e+00_Ti48-q=2.359e+00_Ti48-q=2.424e+00_Ti48-q=5.532e-01_Ti48-q=6.864e-01_Ti48-q=7.680e-01_Ti48-q=8.481e-01_Ti48-q=8.797e-01_Ti48-q=9.111e-01_Ti48-q=9.421e-01_Ti48-q=9.729e-01_Ti48-q=9.883e-01_Ti50-q=1.003e+00_Ti50-q=1.034e+00_Ti50-q=1.038e+00_Ti50-q=1.063e+00_Ti50-q=1.088e+00_Ti50-q=1.093e+00_Ti50-q=1.122e+00_Ti50-q=1.137e+00_Ti50-q=1.151e+00_Ti50-q=1.180e+00_Ti50-q=1.186e+00_Ti50-q=1.208e+00_Ti50-q=1.235e+00_Ti50-q=1.236e+00_Ti50-q=1.263e+00_Ti50-q=1.283e+00_Ti50-q=1.290e+00_Ti50-q=1.317e+00_Ti50-q=1.331e+00_Ti50-q=1.343e+00_Ti50-q=1.369e+00_Ti50-q=1.378e+00_Ti50-q=1.419e+00_Ti50-q=1.425e+00_Ti50-q=1.472e+00_Ti50-q=1.480e+00_Ti50-q=1.518e+00_Ti50-q=1.537e+00_Ti50-q=1.563e+00_Ti50-q=1.592e+00_Ti50-q=1.609e+00_Ti50-q=1.644e+00_Ti50-q=1.653e+00_Ti50-q=1.697e+00_Ti50-q=1.741e+00_Ti50-q=1.784e+00_Ti50-q=1.827e+00_Ti50-q=1.869e+00_Ti50-q=1.910e+00_Ti50-q=1.951e+00_Ti50-q=2.031e+00_Ti50-q=2.070e+00_Ti50-q=2.146e+00_Ti50-q=2.220e+00_Ti50-q=2.291e+00_Ti50-q=2.359e+00_Ti50-q=2.424e+00_Ti50-q=2.487e+00_Ti50-q=5.532e-01_Ti50-q=6.864e-01_Ti50-q=7.680e-01_Ti50-q=8.481e-01_Ti50-q=8.797e-01_Ti50-q=9.111e-01_Ti50-q=9.421e-01_Ti50-q=9.729e-01_Ti50-q=9.883e-01_fermi-Am241_fermi-Am243_fermi-Cd114_fermi-I127_fermi-In115_fermi-Sn116_fermi-Sn124_fermi-Te126_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_fermi-Pb204_fermi-Pb206_fermi-Pb207_fermi-Pb208_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_Cr50-q=-1.161e-01_Cr50-q=-1.244e-01_Cr50-q=-1.260e-01_Cr50-q=-1.327e-01_Cr50-q=-1.410e-01_Cr50-q=-1.440e-01_Cr50-q=-1.490e-01_Cr50-q=-1.580e-01_Cr50-q=-1.740e-01_Cr50-q=-1.820e-01_Cr50-q=-1.910e-01_Cr50-q=-1.990e-01_Cr50-q=-2.070e-01_Cr50-q=-2.160e-01_Cr50-q=-2.250e-01_Cr50-q=-2.320e-01_Cr50-q=-2.430e-01_Cr50-q=-2.490e-01_Cr50-q=-2.610e-01_Cr50-q=-2.650e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.530e-01_Cr50-q=2.633e-01_Cr50-q=2.790e-01_Cr50-q=3.040e-01_Cr50-q=3.072e-01_Cr50-q=3.290e-01_Cr50-q=3.494e-01_Cr50-q=3.511e-01_Cr50-q=3.550e-01_Cr50-q=3.793e-01_Cr50-q=3.798e-01_Cr50-q=3.800e-01_Cr50-q=3.950e-01_Cr50-q=4.050e-01_Cr50-q=4.092e-01_Cr50-q=4.310e-01_Cr50-q=4.389e-01_Cr50-q=4.492e-01_Cr50-q=4.828e-01_Cr50-q=4.991e-01_Cr50-q=5.267e-01_Cr50-q=5.490e-01_Cr50-q=5.705e-01_Cr50-q=5.989e-01_Cr50-q=6.144e-01_Cr50-q=6.488e-01_Cr50-q=6.583e-01_Cr50-q=6.987e-01_Cr50-q=7.022e-01_Cr50-q=7.460e-01_Cr50-q=7.486e-01_Cr50-q=7.985e-01_Cr50-q=8.490e-01_Cr50-q=8.983e-01_Cr50-q=9.482e-01_Cr52-q=-1.161e-01_Cr52-q=-1.244e-01_Cr52-q=-1.260e-01_Cr52-q=-1.327e-01_Cr52-q=-1.410e-01_Cr52-q=-1.440e-01_Cr52-q=-1.580e-01_Cr52-q=-1.660e-01_Cr52-q=-1.710e-01_Cr52-q=-1.740e-01_Cr52-q=-1.820e-01_Cr52-q=-1.910e-01_Cr52-q=-1.990e-01_Cr52-q=-2.070e-01_Cr52-q=-2.160e-01_Cr52-q=-2.250e-01_Cr52-q=-2.320e-01_Cr52-q=-2.430e-01_Cr52-q=-2.490e-01_Cr52-q=-2.610e-01_Cr52-q=-2.650e-01_Cr52-q=-2.790e-01_Cr52-q=1.520e-01_Cr52-q=1.774e-01_Cr52-q=2.027e-01_Cr52-q=2.280e-01_Cr52-q=2.530e-01_Cr52-q=2.633e-01_Cr52-q=2.790e-01_Cr52-q=3.040e-01_Cr52-q=3.072e-01_Cr52-q=3.290e-01_Cr52-q=3.494e-01_Cr52-q=3.511e-01_Cr52-q=3.550e-01_Cr52-q=3.793e-01_Cr52-q=3.798e-01_Cr52-q=3.800e-01_Cr52-q=3.950e-01_Cr52-q=4.050e-01_Cr52-q=4.092e-01_Cr52-q=4.310e-01_Cr52-q=4.389e-01_Cr52-q=4.492e-01_Cr52-q=4.828e-01_Cr52-q=4.991e-01_Cr52-q=5.267e-01_Cr52-q=5.490e-01_Cr52-q=5.705e-01_Cr52-q=5.989e-01_Cr52-q=6.144e-01_Cr52-q=6.488e-01_Cr52-q=6.583e-01_Cr52-q=6.987e-01_Cr52-q=7.022e-01_Cr52-q=7.460e-01_Cr52-q=7.486e-01_Cr52-q=7.985e-01_Cr52-q=8.490e-01_Cr52-q=8.983e-01_Cr52-q=9.482e-01_Cr54-q=-1.161e-01_Cr54-q=-1.244e-01_Cr54-q=-1.260e-01_Cr54-q=-1.327e-01_Cr54-q=-1.410e-01_Cr54-q=-1.440e-01_Cr54-q=-1.580e-01_Cr54-q=-1.710e-01_Cr54-q=-1.740e-01_Cr54-q=-1.820e-01_Cr54-q=-1.910e-01_Cr54-q=-1.990e-01_Cr54-q=-2.070e-01_Cr54-q=-2.160e-01_Cr54-q=-2.250e-01_Cr54-q=-2.320e-01_Cr54-q=-2.430e-01_Cr54-q=-2.490e-01_Cr54-q=-2.610e-01_Cr54-q=-2.650e-01_Cr54-q=-2.790e-01_Cr54-q=1.520e-01_Cr54-q=1.774e-01_Cr54-q=2.027e-01_Cr54-q=2.280e-01_Cr54-q=2.530e-01_Cr54-q=2.633e-01_Cr54-q=2.790e-01_Cr54-q=3.040e-01_Cr54-q=3.072e-01_Cr54-q=3.290e-01_Cr54-q=3.494e-01_Cr54-q=3.511e-01_Cr54-q=3.550e-01_Cr54-q=3.793e-01_Cr54-q=3.798e-01_Cr54-q=3.800e-01_Cr54-q=3.950e-01_Cr54-q=4.050e-01_Cr54-q=4.092e-01_Cr54-q=4.310e-01_Cr54-q=4.389e-01_Cr54-q=4.492e-01_Cr54-q=4.828e-01_Cr54-q=4.991e-01_Cr54-q=5.267e-01_Cr54-q=5.490e-01_Cr54-q=5.705e-01_Cr54-q=5.989e-01_Cr54-q=6.144e-01_Cr54-q=6.488e-01_Cr54-q=6.583e-01_Cr54-q=6.987e-01_Cr54-q=7.022e-01_Cr54-q=7.460e-01_Cr54-q=7.486e-01_Cr54-q=7.985e-01_Cr54-q=8.490e-01_Cr54-q=8.983e-01_Cr54-q=9.482e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.534e-01_Cr50-q=2.633e-01_Cr50-q=2.787e-01_Cr50-q=3.041e-01_Cr50-q=3.072e-01_Cr50-q=3.294e-01_Cr50-q=3.511e-01_Cr50-q=3.547e-01_Cr50-q=3.801e-01_Cr50-q=3.950e-01_Cr50-q=4.054e-01_Cr50-q=4.308e-01_Cr50-q=4.389e-01_Cr50-q=4.828e-01_Cr50-q=5.267e-01_Cr50-q=5.705e-01_Cr50-q=6.144e-01_Cr50-q=6.583e-01_Cr50-q=7.022e-01_Cr50-q=7.461e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.534e-01_Cr50-q=2.633e-01_Cr50-q=2.787e-01_Cr50-q=3.041e-01_Cr50-q=3.072e-01_Cr50-q=3.294e-01_Cr50-q=3.511e-01_Cr50-q=3.547e-01_Cr50-q=3.801e-01_Cr50-q=3.950e-01_Cr50-q=4.054e-01_Cr50-q=4.308e-01_Cr50-q=4.389e-01_Cr50-q=4.828e-01_Cr50-q=5.267e-01_Cr50-q=5.705e-01_Cr50-q=6.144e-01_Cr50-q=6.583e-01_Cr50-q=7.022e-01_Cr50-q=7.461e-01_Cr52-q=1.520e-01_Cr52-q=1.774e-01_Cr52-q=2.027e-01_Cr52-q=2.280e-01_Cr52-q=2.534e-01_Cr52-q=2.633e-01_Cr52-q=2.787e-01_Cr52-q=3.041e-01_Cr52-q=3.072e-01_Cr52-q=3.294e-01_Cr52-q=3.511e-01_Cr52-q=3.547e-01_Cr52-q=3.801e-01_Cr52-q=3.950e-01_Cr52-q=4.054e-01_Cr52-q=4.308e-01_Cr52-q=4.389e-01_Cr52-q=4.828e-01_Cr52-q=5.267e-01_Cr52-q=5.705e-01_Cr52-q=6.144e-01_Cr52-q=6.583e-01_Cr52-q=7.022e-01_Cr52-q=7.461e-01_2s1/2-2p3/2_Zr90-1s1/2_NP-Mixed_2p1/2-1s1/2_2p3/2-1s1/2_Sn112-1s1/2_Sn112-2p1/2_Sn112-2p3/2_NP-Calculated_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_Pb104-2p1/2-1s1/2_Pd104-2p1/2-1s1/2_Pd104-2p3/2-1s1/2_Pd104-3d3/2-2p1/2_Pd104-3d5/2-2p3/2_Pd104-4d5/2-2p3/2_Pd104-4f5/2-3d3/2_Pd104-4f7/2-3d5/2_Pd106-2p1/2-1s1/2_Pd106-2p3/2-1s1/2_Pd106-3d3/2-2p1/2_Pd106-3d5/2-2p3/2_Pd106-4d5/2-2p3/2_Pd106-4f5/2-3d3/2_Pd106-4f7/2-3d5/2_Pd108-2p1/2-1s1/2_Pd108-2p3/2-1s1/2_Pd108-3d3/2-2p1/2_Pd108-3d5/2-2p3/2_Pd108-4d5/2-2p3/2_Pd108-4f5/2-3d3/2_Pd108-4f7/2-3d5/2_Pd110-2p1/2-1s1/2_Pd110-2p3/2-1s1/2_Pd110-3d3/2-2p1/2_Pd110-3d5/2-2p3/2_Pd110-4d5/2-2p3/2_Pd110-4f5/2-3d3/2_Pd110-4f7/2-3d5/2_fermi-Pd104_fermi-Pd106_fermi-Pd108_fermi-Pd110_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p-1s_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_(0+,2p3/2)3/2--(0+,1s1/2)1/2+_(2+,2p3/2)1/2--(2+,1s1/2)3/2+_Pb203-2p1/2-1s1/2_(1+,1s1/2)1/2-(2+,1s1/2)1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_difference-Zr90_Sn112-1s1/2_Sn112-2p1/2_NP-Vary_NP-Calculated_Ca40-2p3/2-1s1/2_Ca42-2p3/2-1s1/2_Ca43-2p3/2-1s1/2_Ca44-2p3/2-1s1/2_Ca46-2p3/2-1s1/2_Ca48-2p3/2-1s1/2_Cr50-2p3/2-1s1/2_Cr52-2p3/2-1s1/2_Cr53-2p3/2-1s1/2_Cr54-2p3/2-1s1/2_Fe56-2p3/2-1s1/2_K39-2p3/2-1s1/2_K41-2p3/2-1s1/2_Mn55-2p3/2-1s1/2_Sc45-2p3/2-1s1/2_Ti46-2p3/2-1s1/2_Ti47-2p3/2-1s1/2_Ti48-2p3/2-1s1/2_Ti49-2p3/2-1s1/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{ + "Reference": "test_test_1700", + "Previous Muonic Measurements": [ + "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2", + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2", + "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2", + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2", + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2", + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2", + "bergem_nuclear_1988_radius_Pb208_NP_Calculated", + "bergem_nuclear_1988_radius_Pb208_NP_Fit", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.010e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.031e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.051e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.071e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.091e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.111e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.150e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.170e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.190e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.228e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.267e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.343e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.400e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.417e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.489e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.520e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.560e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.629e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.650e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.712e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.730e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.792e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.820e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.868e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.900e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.941e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.980e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.010e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.060e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.076e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.137e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.180e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.248e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.300e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.420e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.530e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.650e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=6.980e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=7.620e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=8.140e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=8.670e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.080e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.490e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.695e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=7.830e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.010e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.051e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.091e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.131e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.170e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.228e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.305e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.400e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.520e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.650e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.730e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.820e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.868e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.900e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.941e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.980e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.010e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.060e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.076e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.137e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.180e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.248e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.300e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.420e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.530e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.228e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.305e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.380e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.453e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.525e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.900e-01", + "hahn_experimental_1979_fermi_Hg198", + "hahn_experimental_1979_fermi_Hg199", + "hahn_experimental_1979_fermi_Hg200", + "hahn_experimental_1979_fermi_Hg201", + "hahn_experimental_1979_fermi_Hg202", + "hahn_experimental_1979_fermi_Hg204", + "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg198_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg198_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg200_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg200_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg202_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg202_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg204_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg204_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg199_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg200_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg201_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg202_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg204_1s1/2", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.003e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.034e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.038e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.063e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.088e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.093e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.122e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.137e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.151e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.180e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.186e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.208e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.235e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.236e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.263e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.283e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.290e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.317e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.331e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.343e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.369e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.378e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.419e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.425e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.472e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.480e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.518e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.537e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.563e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.592e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.609e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.653e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.697e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.741e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.784e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.827e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.869e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.910e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.951e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.031e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.070e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.146e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.220e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.291e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.359e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.424e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=5.532e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=6.864e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=7.680e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.481e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.797e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.111e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.421e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.729e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.883e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.003e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.034e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.038e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.063e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.088e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.093e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.122e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.137e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.151e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.180e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.186e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.208e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.235e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.236e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.263e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.283e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.290e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.317e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.331e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.343e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.369e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.378e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.419e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.425e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.472e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.480e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.518e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.537e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.563e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.592e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.609e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.644e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.653e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.697e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.741e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.784e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.827e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.869e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.910e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.951e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.031e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.070e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.146e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.220e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.291e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.359e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.424e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.487e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=5.532e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=6.864e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=7.680e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.481e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.797e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.111e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.421e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.729e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.883e-01", + "johnson_241am_1985_fermi_Am241", + "johnson_241am_1985_fermi_Am243", + "kast_isotone_1971_fermi_Cd114", + "kast_isotone_1971_fermi_I127", + "kast_isotone_1971_fermi_In115", + "kast_isotone_1971_fermi_Sn116", + "kast_isotone_1971_fermi_Sn124", + "kast_isotone_1971_fermi_Te126", + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_I127_2p1/2_1s1/2", + "kast_isotone_1971_muonic_I127_2p3/2_1s1/2", + "kast_isotone_1971_muonic_I127_3d3/2_2p1/2", + "kast_isotone_1971_muonic_I127_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2", + "kast_isotone_1971_radius_Cd114_NP_Calculated", + "kast_isotone_1971_radius_I127_NP_Calculated", + "kast_isotone_1971_radius_In115_NP_Calculated", + "kast_isotone_1971_radius_Sn116_NP_Calculated", + "kast_isotone_1971_radius_Sn124_NP_Calculated", + "kast_isotone_1971_radius_Te126_NP_Calculated", + "kessler_muonic_1975_fermi_Pb204", + "kessler_muonic_1975_fermi_Pb206", + "kessler_muonic_1975_fermi_Pb207", + "kessler_muonic_1975_fermi_Pb208", + "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_radius_Pb204_NP_Calculated", + "kessler_muonic_1975_radius_Pb206_NP_Calculated", + "kessler_muonic_1975_radius_Pb207_NP_Calculated", + "kessler_muonic_1975_radius_Pb208_NP_Calculated", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.660e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.710e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.710e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.461e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.461e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.461e-01", + "phan_nuclear_1985_muonic_Zr90_2s1/2_2p3/2", + "phan_nuclear_1985_muonic_nuclear_polarization_Zr90_1s1/2", + "phan_nuclear_1985_radius_Zr90_NP_Mixed", + "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2", + "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2", + "piller_nuclear_1990_radius_Sn112_NP_Calculated", + "powers_hyperfine_1968_muonic_Bi209_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_2p1/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_3d3/2_2p1/2", + "powers_hyperfine_1968_muonic_Pb206_3d5/2_2p3/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p1/2_1s1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d3/2_2p1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d5/2_2p3/2", + "saito_muonic_2025_barrett_moment_Pb104_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd104_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd104_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd104_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd104_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd106_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd106_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd106_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd106_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd106_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd106_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd106_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd108_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd108_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd108_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd108_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd108_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd108_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd108_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd110_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd110_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd110_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd110_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd110_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd110_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd110_4f7/2-3d5/2", + "saito_muonic_2025_fermi_Pd104", + "saito_muonic_2025_fermi_Pd106", + "saito_muonic_2025_fermi_Pd108", + "saito_muonic_2025_fermi_Pd110", + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2", + "schaller_nuclear_1985_muonic_P31_2p_1s", + "shera_systematics_1976_muonic_Co59_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe54_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe56_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe57_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe58_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni58_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni60_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe56_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe56_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe57_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn70_2p3/2_1s1/2", + "tanaka_measurement_1984_muonic_Hf176_(0+,2p3/2)3/2-_(0+,1s1/2)1/2+", + "tanaka_measurement_1984_muonic_Hf176_(2+,2p3/2)1/2-_(2+,1s1/2)3/2+", + "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2", + "test_test_1700_muonic_Pb203_(1+,1s1/2)1/2_(2+,1s1/2)1/2", + "test_test_1700_muonic_Sn112_2p1/2_1s1/2", + "test_test_1700_muonic_difference_Fe1_Fe3_2p3/2_1s1/2", + "test_test_1700_muonic_difference_Fe2_Fe4_2p3/2_1s1/2", + "test_test_1700_muonic_difference_Zr90", + "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", + "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2", + "test_test_1700_radius_Pb203_NP_Vary", + "test_test_1700_radius_Pb204_NP_Calculated", + "wolfhahrt_nuclear_1981_barrett_moment_Ca40_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca42_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca43_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca44_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca46_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca48_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr50_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr52_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr53_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr54_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Fe56_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_K39_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_K41_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Mn55_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Sc45_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti46_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti47_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti48_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti49_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti50_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_V51_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_fermi_Ca40", + "wolfhahrt_nuclear_1981_fermi_Ca42", + "wolfhahrt_nuclear_1981_fermi_Ca43", + "wolfhahrt_nuclear_1981_fermi_Ca44", + "wolfhahrt_nuclear_1981_fermi_Ca46", + "wolfhahrt_nuclear_1981_fermi_Ca48", + "wolfhahrt_nuclear_1981_fermi_Cr50", + "wolfhahrt_nuclear_1981_fermi_Cr52", + "wolfhahrt_nuclear_1981_fermi_Cr53", + "wolfhahrt_nuclear_1981_fermi_Cr54", + "wolfhahrt_nuclear_1981_fermi_Fe56", + "wolfhahrt_nuclear_1981_fermi_K39", + "wolfhahrt_nuclear_1981_fermi_K41", + "wolfhahrt_nuclear_1981_fermi_Mn55", + "wolfhahrt_nuclear_1981_fermi_Sc45", + "wolfhahrt_nuclear_1981_fermi_Ti46", + "wolfhahrt_nuclear_1981_fermi_Ti47", + "wolfhahrt_nuclear_1981_fermi_Ti48", + "wolfhahrt_nuclear_1981_fermi_Ti49", + "wolfhahrt_nuclear_1981_fermi_Ti50", + "wolfhahrt_nuclear_1981_fermi_V51", + "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca48_2p3/2_1s1/2", + 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"wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" + ], + "Nuclide": "P32", + "Rka [fm]": { + "Value": 0.0, + "Uncertainty": null + }, + "k [-]": "0", + "alpha [1/fm]": "0", + "Cz [fm/keV]": "0", + "Nuclear Polarization Method": "Calculated", + "Calculated Nuclear Polarization": [ + "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2", + "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", + "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", + "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2", + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2", + "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2", + "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2", + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2", + "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2", + "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2", + "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2", + "bergem_nuclear_1988_radius_Pb208_NP_Calculated", + "bergem_nuclear_1988_radius_Pb208_NP_Fit", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.010e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.031e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.051e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.071e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.091e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.111e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.150e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.170e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.190e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.228e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.267e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.343e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.400e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.417e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.489e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.520e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.560e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.629e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.650e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.712e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.730e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.792e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.820e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.868e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.900e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.941e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=1.980e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.010e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.060e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.076e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.137e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.180e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.248e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.300e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.420e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.530e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=2.650e+00", + "frosch_electron_1968_electroncrosssection_Ca40_q=6.980e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=7.620e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=8.140e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=8.670e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.080e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.490e-01", + "frosch_electron_1968_electroncrosssection_Ca40_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.695e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=7.830e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.010e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.051e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.091e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.131e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.170e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.228e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.305e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.400e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.520e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.650e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.730e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.820e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.868e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.900e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.941e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.980e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.010e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.060e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.076e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.137e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.180e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.248e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.300e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.420e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.530e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.900e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.031e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.071e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.111e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.150e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.190e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.228e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.267e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.305e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.343e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.380e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.417e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.453e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.489e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.525e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.560e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.629e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.712e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.792e+00", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=6.980e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=7.620e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.140e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.670e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.080e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.490e-01", + "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.900e-01", + "hahn_experimental_1979_fermi_Hg198", + "hahn_experimental_1979_fermi_Hg199", + "hahn_experimental_1979_fermi_Hg200", + "hahn_experimental_1979_fermi_Hg201", + "hahn_experimental_1979_fermi_Hg202", + "hahn_experimental_1979_fermi_Hg204", + "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg198_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg198_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg200_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg200_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg202_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg202_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2", + "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2", + "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2", + "hahn_experimental_1979_muonic_Hg204_4f5/2_3d3/2", + "hahn_experimental_1979_muonic_Hg204_4f7/2_3d5/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg199_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg200_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg201_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg202_1s1/2", + "hahn_experimental_1979_muonic_difference_Hg198_Hg204_1s1/2", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.003e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.034e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.038e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.063e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.088e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.093e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.122e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.137e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.151e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.180e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.186e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.208e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.235e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.236e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.263e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.283e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.290e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.317e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.331e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.343e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.369e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.378e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.419e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.425e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.472e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.480e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.518e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.537e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.563e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.592e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.609e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.653e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.697e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.741e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.784e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.827e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.869e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.910e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.951e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.031e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.070e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.146e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.220e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.291e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.359e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.424e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=5.532e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=6.864e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=7.680e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.481e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.797e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.111e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.421e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.729e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.883e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.003e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.034e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.038e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.063e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.088e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.093e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.122e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.137e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.151e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.180e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.186e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.208e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.235e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.236e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.263e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.283e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.290e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.317e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.331e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.343e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.369e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.378e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.419e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.425e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.472e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.480e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.518e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.537e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.563e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.592e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.609e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.644e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.653e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.697e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.741e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.784e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.827e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.869e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.910e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.951e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.031e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.070e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.146e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.220e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.291e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.359e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.424e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.487e+00", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=5.532e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=6.864e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=7.680e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.481e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.797e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.111e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.421e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.729e-01", + "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.883e-01", + "johnson_241am_1985_fermi_Am241", + "johnson_241am_1985_fermi_Am243", + "kast_isotone_1971_fermi_Cd114", + "kast_isotone_1971_fermi_I127", + "kast_isotone_1971_fermi_In115", + "kast_isotone_1971_fermi_Sn116", + "kast_isotone_1971_fermi_Sn124", + "kast_isotone_1971_fermi_Te126", + "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", + "kast_isotone_1971_muonic_I127_2p1/2_1s1/2", + "kast_isotone_1971_muonic_I127_2p3/2_1s1/2", + "kast_isotone_1971_muonic_I127_3d3/2_2p1/2", + "kast_isotone_1971_muonic_I127_3d5/2_2p3/2", + "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", + "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", + "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", + "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", + "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", + "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", + "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", + "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2", + "kast_isotone_1971_radius_Cd114_NP_Calculated", + "kast_isotone_1971_radius_I127_NP_Calculated", + "kast_isotone_1971_radius_In115_NP_Calculated", + "kast_isotone_1971_radius_Sn116_NP_Calculated", + "kast_isotone_1971_radius_Sn124_NP_Calculated", + "kast_isotone_1971_radius_Te126_NP_Calculated", + "kessler_muonic_1975_fermi_Pb204", + "kessler_muonic_1975_fermi_Pb206", + "kessler_muonic_1975_fermi_Pb207", + "kessler_muonic_1975_fermi_Pb208", + "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", + "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", + "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", + "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", + "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb204_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb206_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb207_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_2s1/2_2p1/2_B_2s1/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_3d5/2_2p3/2_B_3d3/2_2p3/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", + "kessler_muonic_1975_muonic_difference_Pb208_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", + "kessler_muonic_1975_radius_Pb204_NP_Calculated", + "kessler_muonic_1975_radius_Pb206_NP_Calculated", + "kessler_muonic_1975_radius_Pb207_NP_Calculated", + "kessler_muonic_1975_radius_Pb208_NP_Calculated", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr50_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.660e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.710e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr52_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.161e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.244e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.260e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.327e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.410e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.440e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.580e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.710e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.740e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.820e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.910e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.990e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.070e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.160e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.250e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.320e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.430e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.610e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.650e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.530e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.790e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.040e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.290e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.494e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.550e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.793e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.798e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.800e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.050e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.092e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.310e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.492e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.991e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.989e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.488e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.987e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.460e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.486e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.985e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.490e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.983e-01", + "lightbody_elastic_1983_electroncrosssection_Cr54_q=9.482e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.461e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.461e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.520e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.774e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.027e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.280e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.534e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.633e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.787e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.041e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.072e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.294e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.511e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.547e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.801e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.950e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.054e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.308e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.389e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.828e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.267e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.705e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.144e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.583e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.022e-01", + "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.461e-01", + "phan_nuclear_1985_muonic_Zr90_2s1/2_2p3/2", + "phan_nuclear_1985_muonic_nuclear_polarization_Zr90_1s1/2", + "phan_nuclear_1985_radius_Zr90_NP_Mixed", + "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2", + "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2", + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2", + "piller_nuclear_1990_radius_Sn112_NP_Calculated", + "powers_hyperfine_1968_muonic_Bi209_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_2p1/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_Pb206_3d3/2_2p1/2", + "powers_hyperfine_1968_muonic_Pb206_3d5/2_2p3/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p1/2_1s1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p3/2_1s1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d3/2_2p1/2", + "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d5/2_2p3/2", + "saito_muonic_2025_barrett_moment_Pb104_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd104_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd104_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd104_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd104_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd104_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd106_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd106_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd106_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd106_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd106_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd106_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd106_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd108_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd108_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd108_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd108_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd108_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd108_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd108_4f7/2-3d5/2", + "saito_muonic_2025_barrett_moment_Pd110_2p1/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd110_2p3/2-1s1/2", + "saito_muonic_2025_barrett_moment_Pd110_3d3/2-2p1/2", + "saito_muonic_2025_barrett_moment_Pd110_3d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd110_4d5/2-2p3/2", + "saito_muonic_2025_barrett_moment_Pd110_4f5/2-3d3/2", + "saito_muonic_2025_barrett_moment_Pd110_4f7/2-3d5/2", + "saito_muonic_2025_fermi_Pd104", + "saito_muonic_2025_fermi_Pd106", + "saito_muonic_2025_fermi_Pd108", + "saito_muonic_2025_fermi_Pd110", + "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2", + "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2", + "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2", + "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2", + "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2", + "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2", + "schaller_nuclear_1985_muonic_P31_2p_1s", + "shera_systematics_1976_muonic_Co59_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe54_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe56_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe57_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Fe58_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni58_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni60_2p1/2_1s1/2", + "shera_systematics_1976_muonic_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Co59_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu63_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Cu65_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe54_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe56_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe56_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Fe57_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni58_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni60_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni61_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni62_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Ni64_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn64_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn66_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn68_Zn70_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_difference_Zn70_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Co59_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Cu63_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Cu65_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe54_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe57_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Fe58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni58_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni60_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni61_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni62_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Ni64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn64_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn66_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn68_2p3/2_1s1/2", + "shera_systematics_1976_muonic_nuclear_polarization_Zn70_2p3/2_1s1/2", + "tanaka_measurement_1984_muonic_Hf176_(0+,2p3/2)3/2-_(0+,1s1/2)1/2+", + "tanaka_measurement_1984_muonic_Hf176_(2+,2p3/2)1/2-_(2+,1s1/2)3/2+", + "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2", + "test_test_1700_muonic_Pb203_(1+,1s1/2)1/2_(2+,1s1/2)1/2", + "test_test_1700_muonic_Sn112_2p1/2_1s1/2", + "test_test_1700_muonic_difference_Fe1_Fe3_2p3/2_1s1/2", + "test_test_1700_muonic_difference_Fe2_Fe4_2p3/2_1s1/2", + "test_test_1700_muonic_difference_Zr90", + "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", + "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2", + "test_test_1700_radius_Pb203_NP_Vary", + "test_test_1700_radius_Pb204_NP_Calculated", + "wolfhahrt_nuclear_1981_barrett_moment_Ca40_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca42_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca43_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca44_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca46_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ca48_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr50_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr52_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr53_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Cr54_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Fe56_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_K39_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_K41_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Mn55_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Sc45_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti46_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti47_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti48_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti49_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_Ti50_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_barrett_moment_V51_2p3/2-1s1/2", + "wolfhahrt_nuclear_1981_fermi_Ca40", + "wolfhahrt_nuclear_1981_fermi_Ca42", + "wolfhahrt_nuclear_1981_fermi_Ca43", + "wolfhahrt_nuclear_1981_fermi_Ca44", + "wolfhahrt_nuclear_1981_fermi_Ca46", + "wolfhahrt_nuclear_1981_fermi_Ca48", + "wolfhahrt_nuclear_1981_fermi_Cr50", + "wolfhahrt_nuclear_1981_fermi_Cr52", + "wolfhahrt_nuclear_1981_fermi_Cr53", + "wolfhahrt_nuclear_1981_fermi_Cr54", + "wolfhahrt_nuclear_1981_fermi_Fe56", + "wolfhahrt_nuclear_1981_fermi_K39", + "wolfhahrt_nuclear_1981_fermi_K41", + "wolfhahrt_nuclear_1981_fermi_Mn55", + "wolfhahrt_nuclear_1981_fermi_Sc45", + "wolfhahrt_nuclear_1981_fermi_Ti46", + "wolfhahrt_nuclear_1981_fermi_Ti47", + "wolfhahrt_nuclear_1981_fermi_Ti48", + "wolfhahrt_nuclear_1981_fermi_Ti49", + "wolfhahrt_nuclear_1981_fermi_Ti50", + "wolfhahrt_nuclear_1981_fermi_V51", + "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr50_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr52_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr53_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Cr54_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Fe56_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_K41_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Mn55_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2", + "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" + ], + "Notes": "" } } diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy.json b/radbase/compilation/test_test_1700/Muonic Transition Energy.json index 6696b99..c021a14 100644 --- a/radbase/compilation/test_test_1700/Muonic Transition Energy.json +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy.json @@ -11,5 +11,18 @@ "uncertainty": 0.06 }, "Notes": "" + }, + "test_test_1700_muonic_Pb203_(1+,1s1/2)1/2_(2+,1s1/2)1/2": { + "Reference": "test_test_1700", + "Nuclide": "Pb203", + "Transition": { + "Upper": "(1+,1s1/2)1/2", + "Lower": "(2+,1s1/2)1/2" + }, + "Energy [keV]": { + "Value": 100.0, + "Uncertainty": 1.0 + }, + "Notes": "" } } diff --git a/radbase/data_entry.py b/radbase/data_entry.py index d88fe40..313146d 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -219,11 +219,11 @@ def process(self, widget: tk.Widget): def process_data(self, data): try: value = float(data) - return {self.key: {'value': value, 'uncertainty': None}} + return {self.key: {'Value': value, 'Uncertainty': None}} except ValueError: try: uvar = uncertainties.ufloat_fromstr(data) - return {self.key: {'value': uvar.n, 'uncertainty': uvar.s}} + return {self.key: {'Value': uvar.n, 'Uncertainty': uvar.s}} except ValueError: raise ValueError( f'Entered value of {data} does not match the number with uncertainty pattern. Ex. 0.65(2) or 0.32') @@ -239,8 +239,7 @@ def __init__(self): self.varied_processor = VariableNumberProcessor( GroupedProcessor([ XORProcessor( - [TransitionProcessor(), CastProcessor(str, key='Level')] - ), + [TransitionProcessor(), CastProcessor(str, key='Level')]), NumberWithUncertaintyProcessor('Energy [keV]') ])) @@ -265,11 +264,11 @@ def process_data(self, data): result = {'Nuclear Polarization Method': mode} if mode == 'Calculated': - return result | self.calced_processor.process(calced_data) + return result | self.calced_processor.process_data(calced_data) elif mode == 'Vary': - return result | self.varied_processor.process(fit_data) + return result | self.varied_processor.process_data(fit_data) elif mode == 'Mixed': - return result | self.calced_processor.process(calced_data) | self.varied_processor.process(fit_data) + return result | self.calced_processor.process_data(calced_data) | self.varied_processor.process_data(fit_data) else: raise ValueError(f'{mode} is not in [Calculated, Vary, Mixed]') @@ -284,7 +283,7 @@ def process(self, widget: tk.Widget): return self.process_data(self.unpack_widget(widget)) def unpack_widget(self, widget: tk.Widget) -> list: - return [self.processor.unpack_widget(sub_widget) for sub_widget in widget.entries] + return [self.processor.unpack_widget(sub_widget) for _, sub_widget in widget.entries] def process_data(self, data): data = {} @@ -334,14 +333,10 @@ def process(self, widget: tk.Widget) -> dict[str, list[str]]: @staticmethod def unpack_widget(widget: tk.Widget): - return widget.selection_vars.items() + return {key: checkbox for key, checkbox in widget.selection_vars.items()} def process_data(self, data: dict) -> dict[str, list[str]]: - selected = [ - key - for key, var in data.items() - if var.get() - ] + selected = [key for key, var in data.items() if var] return {self.key: selected} @@ -416,6 +411,21 @@ class TransitionProcessor: re.VERBOSE ) + HYBRID_F_LEVEL_PATTERN = re.compile( + r""" + ^ + \( + \d+[+-], # nuclear spin/parity (e.g. 2+, 0-) + \d+ # principal quantum number + [spdf] # orbital + \d/\d # required j + \) + \d/\d[+-] + $ + """, + re.VERBOSE + ) + def __init__(self, key: str = 'Transition'): self.key = key @@ -440,15 +450,19 @@ def process_data(self, data) -> dict[str, dict[str, str]]: upper_hybrid = self.HYBRID_LEVEL_PATTERN.match(upper) lower_hybrid = self.HYBRID_LEVEL_PATTERN.match(lower) + upper_hybrid_with_f = self.HYBRID_F_LEVEL_PATTERN.match(upper) + lower_hybrid_with_f = self.HYBRID_F_LEVEL_PATTERN.match(lower) + # both simple or both hybrid - if upper_simple and lower_simple or upper_hybrid and lower_hybrid: + if upper_simple and lower_simple or upper_hybrid and lower_hybrid or upper_hybrid_with_f and lower_hybrid_with_f: return {self.key: {'Upper': upper, 'Lower': lower}} raise ValueError( "Invalid transition format.\n" "Both levels must be either:\n" " - Simple atomic levels (e.g. 2p3/2)\n" - " - Hybrid nuclear+atomic levels (e.g. 2+,1s1/2)" + " - Hybrid nuclear+atomic levels (e.g. 2+,1s1/2)\n" + " - Hybrid nuclear+atomic levels with F (e.g. (0+,1s1/2)1/2" ) @@ -979,6 +993,10 @@ class InputTemplate(NamedTuple): fields: list[FieldSpec] data_key: Callable[[dict[str, Any]], str] + @property + def proc_dict(self) -> dict[str, FieldProcessor]: + return {field.label: field.processor for field in self.fields} + # Useful fields that get reused reference_field = FieldSpec("Reference", ReferenceProcessor(reference_path=config['reference_path']), @@ -1021,7 +1039,7 @@ class InputTemplate(NamedTuple): notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'muonic_difference', values['Nuclide_A'], values['Nuclide_B'], + [values['Reference'], 'muonicdifference', values['Nuclide_A'], values['Nuclide_B'], *([values['Transition']['Upper'], values['Transition']['Lower']] if 'Transition' in values else [ values['Level'], ])]) ) @@ -1041,7 +1059,7 @@ class InputTemplate(NamedTuple): notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'muonic_difference', values['Nuclide'], + [values['Reference'], 'muonicdifference', values['Nuclide'], *list( sum([(field_name, field['Upper'], field['Lower']) for field_name, field in values.items() if 'Transition' in field_name.lower()], @@ -1051,10 +1069,10 @@ class InputTemplate(NamedTuple): def mu_nuc_pol_key(values): if 'Transition' in values: - return '_'.join([values['Reference'], 'muonic_nuclear_polarization', values['Nuclide'], + return '_'.join([values['Reference'], 'muonicnuclearpolarization', values['Nuclide'], values['Transition']['Upper'], values['Transition']['Lower']]) else: - return '_'.join([values['Reference'], 'muonic_nuclear_polarization', values['Nuclide'], + return '_'.join([values['Reference'], 'muonicnuclearpolarization', values['Nuclide'], values['Level']]) @@ -1072,10 +1090,10 @@ def mu_nuc_pol_key(values): def mu_nuc_pol_key(values): if 'Transition' in values: - return '_'.join([values['Reference'], 'muonic_qed', values['Nuclide'], + return '_'.join([values['Reference'], 'muonicqed', values['Nuclide'], values['Transition']['Upper'], values['Transition']['Lower']]) else: - return '_'.join([values['Reference'], 'muonic_qed', values['Nuclide'], + return '_'.join([values['Reference'], 'muonicqed', values['Nuclide'], values['Level']]) @@ -1108,7 +1126,7 @@ def mu_nuc_pol_key(values): hovertext='Were the NP corrections from theory ("Calculated") or varied as part of the optimization ("Fit")?'), notes_field ], - data_key=lambda values: '_'.join([values['Reference'], 'barrett_moment', values['Nuclide'], + data_key=lambda values: '_'.join([values['Reference'], 'barrettmoment', values['Nuclide'], *['-'.join(s.split('_')[-2:]) for s in values['Previous Muonic Measurements']]]) ) @@ -1136,7 +1154,7 @@ def mu_nuc_pol_key(values): notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'barrett_moment_difference', values['Nuclide_A'], values['Nuclide_B'], + [values['Reference'], 'barrettmomentdifference', values['Nuclide_A'], values['Nuclide_B'], *['-'.join(s.split('_')[-2:]) for s in values['Previous Muonic Measurements']]]) ) @@ -1185,13 +1203,13 @@ def mu_nuc_pol_key(values): reference_field, nuclide_field, FieldSpec('q [1/fm]', NumberWithUncertaintyProcessor(key='q [1/fm]')), - FieldSpec('E [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), + FieldSpec('Energy [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), FieldSpec('theta [deg]', NumberWithUncertaintyProcessor(key='theta [deg]')), - FieldSpec('Cross section [μb/sr]', NumberWithUncertaintyProcessor(key='Cross section [μb/sr]')), + FieldSpec('Cross section [fm^2/sr]', NumberWithUncertaintyProcessor(key='Cross section [fm^2/sr]')), notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'electron_cross_section', values['Nuclide'], f'q={values['q [1/fm]']['Value']:0.3e}']) + [values['Reference'], 'electroncrosssection', values['Nuclide'], f'q={values['q [1/fm]']['Value']:0.3e}']) ) electron_scattering_cross_section_ratio_template = InputTemplate( @@ -1201,13 +1219,13 @@ def mu_nuc_pol_key(values): FieldSpec("Nuclide A", NuclideProcessor(key="Nuclide_A")), FieldSpec("Nuclide B", NuclideProcessor(key="Nuclide_B")), FieldSpec('q [1/fm]', NumberWithUncertaintyProcessor(key='q [1/fm]')), - FieldSpec('E [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), + FieldSpec('Energy [MeV]', NumberWithUncertaintyProcessor(key='E [MeV]')), FieldSpec('theta [deg]', NumberWithUncertaintyProcessor(key='theta [deg]')), - FieldSpec('Cross section Ratio (A/B) [μb/sr]', NumberWithUncertaintyProcessor(key='Cross section [μb/sr]')), + FieldSpec('Cross section ratio (A/B) [-]', NumberWithUncertaintyProcessor(key='Cross section Ratio [-]')), notes_field ], data_key=lambda values: '_'.join( - [values['Reference'], 'electron_cross_section_ratio', values['Nuclide_A'], values['Nuclide_B'], + [values['Reference'], 'electroncrosssectionratio', values['Nuclide_A'], values['Nuclide_B'], f'q={values['q [1/fm]']['Value']:0.3e}']) ) @@ -1220,7 +1238,8 @@ def mu_nuc_pol_key(values): muonic_barret_shift_template, muonic_radius_template, muonic_fermi_distribution_template, - electron_scattering_cross_section_template] + electron_scattering_cross_section_template, + electron_scattering_cross_section_ratio_template] class DataEntryInterface: diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py index 3536626..47469f4 100644 --- a/tests/test_data_entry.py +++ b/tests/test_data_entry.py @@ -8,8 +8,8 @@ GroupedProcessor, InputTemplate, NuclideProcessor, NumberWithUncertaintyProcessor, - ReferenceProcessor, TransitionProcessor, - XORProcessor) + PreviousDataProcessor, ReferenceProcessor, + TransitionProcessor, XORProcessor) if os.environ.get('DISPLAY', '') == '': print('no display found. Using :0.0') @@ -33,8 +33,6 @@ 'Reference': list(example_references.keys())[0], 'Previous Muonic Measurements': list(example_references.keys())[0] + '_muonic_2p1/2_1s1/2', 'Nuclide': 'Pb208' - '' - } @@ -105,6 +103,17 @@ def test_reference_processor(tmp_path): ref_proc.process(bad_widget) +def test_previous_data_processor(tmp_path): + options = {'test_test_0000_data1': True, + 'test_test_0000_data2': False} + + previous_widget = DummyWidget('') + previous_widget.selection_vars = options + + prev_data_proc = PreviousDataProcessor(key='test') + assert prev_data_proc.process(previous_widget) == {'test': ['test_test_0000_data1']} + + def test_number_with_uncertainty_processor(): float_widget = DummyWidget('100.1') uncertainty_widget = DummyWidget('100.1(3)') @@ -112,8 +121,8 @@ def test_number_with_uncertainty_processor(): ref_proc = NumberWithUncertaintyProcessor('test') - assert ref_proc.process(float_widget) == {'test': {'value': 100.1, 'uncertainty': None}} - assert ref_proc.process(uncertainty_widget) == {'test': {'value': 100.1, 'uncertainty': 0.3}} + assert ref_proc.process(float_widget) == {'test': {'Value': 100.1, 'Uncertainty': None}} + assert ref_proc.process(uncertainty_widget) == {'test': {'Value': 100.1, 'Uncertainty': 0.3}} with pytest.raises(ValueError) as e_info: ref_proc.process(bad_widget) @@ -175,6 +184,9 @@ def test_transition_processor(): nuclear_upper = DummyWidget('2+,2p1/2') nuclear_lower = DummyWidget('0+,1s1/2') + nuclearf_upper = DummyWidget('(2+,2p1/2)1/2+') + nuclearf_lower = DummyWidget('(0+,1s1/2)1/2-') + trans_widget.upper_entry, trans_widget.lower_entry = simple_upper, simple_lower assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2p', 'Lower': '1s'}} @@ -184,6 +196,9 @@ def test_transition_processor(): trans_widget.upper_entry, trans_widget.lower_entry = nuclear_upper, nuclear_lower assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2+,2p1/2', 'Lower': '0+,1s1/2'}} + trans_widget.upper_entry, trans_widget.lower_entry = nuclearf_upper, nuclearf_lower + assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '(2+,2p1/2)1/2+', 'Lower': '(0+,1s1/2)1/2-'}} + with pytest.raises(ValueError) as e_info: trans_widget.upper_entry, trans_widget.lower_entry = bad_level, bad_level TransitionProcessor().process(trans_widget) @@ -192,17 +207,6 @@ def test_transition_processor(): TransitionProcessor().process(trans_widget) - -# def test_init_data_entry_interface(tmp_path): -# -# global example_references -# -# temp_references_file = tmp_path / 'references.json' -# temp_references_file.write_text(json.dumps(example_references)) -# -# DataEntryInterface() - - def test_save_data(tmp_path): ref_key = list(example_references.keys())[0] test_data = {'Reference': ref_key, 'testfield': 3} From 3ee5bf17a732c48b7bf0bafecf56b8609486d9cc Mon Sep 17 00:00:00 2001 From: Hunter Date: Sun, 22 Feb 2026 15:20:33 -0500 Subject: [PATCH 10/11] Added tests for VariableNumberProcessor issue --- ...gy Difference (different transitions).json | 18 ++++++++ radbase/data_entry.py | 10 +++-- tests/test_data_entry.py | 45 +++++++++++++++++-- 3 files changed, 67 insertions(+), 6 deletions(-) diff --git a/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json index 80b4a75..e27c55a 100644 --- a/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json +++ b/radbase/compilation/test_test_1700/Muonic Transition Energy Difference (different transitions).json @@ -15,5 +15,23 @@ "uncertainty": null }, "Notes": "" + }, + "test_test_1700_muonicdifference_W174": { + "Reference": "test_test_1700", + "Nuclide": "W174", + "Energy Difference [keV] (A-B)": { + "Value": 100.0, + "Uncertainty": null + }, + "Notes": "" + }, + "test_test_1700_muonicdifference_pb203": { + "Reference": "test_test_1700", + "Nuclide": "pb203", + "Energy Difference [keV] (A-B)": { + "Value": 100.0, + "Uncertainty": null + }, + "Notes": "" } } diff --git a/radbase/data_entry.py b/radbase/data_entry.py index 313146d..e8bc2a0 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -286,12 +286,16 @@ def unpack_widget(self, widget: tk.Widget) -> list: return [self.processor.unpack_widget(sub_widget) for _, sub_widget in widget.entries] def process_data(self, data): - data = {} + result = {} + + if len(self.suffixes) < len(data): + raise ValueError(f'Not enough suffixes for data. {len(self.suffixes)} suffixes and {len(data)=}') + for suffix, sub_data in zip(self.suffixes, data): sub_result = self.processor.process_data(sub_data) sub_result = {key + suffix: value for key, value in sub_result.items()} - data = data | sub_result - return data + result = result | sub_result + return result class MultiTransitionProcessor: diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py index 47469f4..c07edbb 100644 --- a/tests/test_data_entry.py +++ b/tests/test_data_entry.py @@ -6,10 +6,11 @@ from radbase.data_entry import (CastProcessor, DataEntryInterface, FieldSpec, GroupedProcessor, InputTemplate, - NuclideProcessor, + NuclearPolarizationProcessor, NuclideProcessor, NumberWithUncertaintyProcessor, PreviousDataProcessor, ReferenceProcessor, - TransitionProcessor, XORProcessor) + TransitionProcessor, VariableNumberProcessor, + XORProcessor) if os.environ.get('DISPLAY', '') == '': print('no display found. Using :0.0') @@ -170,6 +171,16 @@ def test_grouped_processor(): assert grouped_proc.process(parent_widget) == {'label1': 'test', 'label2': 'test'} +def test_variable_number_processor(): + varied_widget = DummyWidget('') + varied_widget.entries = [(None, DummyWidget(str(i))) for i in range(3)] + + var_proc = VariableNumberProcessor(CastProcessor(str, key='test'), suffixes=['_A', '_B', '_C']) + assert var_proc.process(varied_widget) == {'test_A': '0', + 'test_B': '1', + 'test_C': '2'} + + def test_transition_processor(): trans_widget = DummyWidget('') @@ -197,7 +208,8 @@ def test_transition_processor(): assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '2+,2p1/2', 'Lower': '0+,1s1/2'}} trans_widget.upper_entry, trans_widget.lower_entry = nuclearf_upper, nuclearf_lower - assert TransitionProcessor().process(trans_widget) == {'Transition': {'Upper': '(2+,2p1/2)1/2+', 'Lower': '(0+,1s1/2)1/2-'}} + assert TransitionProcessor().process(trans_widget) == { + 'Transition': {'Upper': '(2+,2p1/2)1/2+', 'Lower': '(0+,1s1/2)1/2-'}} with pytest.raises(ValueError) as e_info: trans_widget.upper_entry, trans_widget.lower_entry = bad_level, bad_level @@ -207,6 +219,33 @@ def test_transition_processor(): TransitionProcessor().process(trans_widget) +def test_nuclear_polarization_processor(): + data = {} + data['mode'] = 'Calculated' + data['fit_data'] = [[({'Upper': '', 'Lower': ''}, '1s'), '30.3']] + data['calced_data'] = {'test_ref_1': True, 'test_ref_2': False} + + assert NuclearPolarizationProcessor().process_data(data) == {'Nuclear Polarization Method': 'Calculated', + 'Calculated Nuclear Polarization': + ['test_ref_1']} + + data['mode'] = 'Vary' + assert NuclearPolarizationProcessor().process_data(data) == {'Nuclear Polarization Method': 'Vary', + 'Energy [keV]_A': {'Value': 30.3, + 'Uncertainty': None}, + 'Level_A': '1s' + } + + data['mode'] = 'Mixed' + assert NuclearPolarizationProcessor().process_data(data) == {'Nuclear Polarization Method': 'Mixed', + 'Energy [keV]_A': {'Value': 30.3, + 'Uncertainty': None}, + 'Level_A': '1s', + 'Calculated Nuclear Polarization': + ['test_ref_1'] + } + + def test_save_data(tmp_path): ref_key = list(example_references.keys())[0] test_data = {'Reference': ref_key, 'testfield': 3} From e6cd4ec594be10878568066560ba46b8ad3202a8 Mon Sep 17 00:00:00 2001 From: Hunter Date: Mon, 23 Feb 2026 13:28:20 -0500 Subject: [PATCH 11/11] Fixed PreviousDataProcessor --- .../test_test_1700/Muonic Barrett Moment.json | 2607 +---------------- radbase/data_entry.py | 2 +- tests/test_data_entry.py | 7 +- 3 files changed, 10 insertions(+), 2606 deletions(-) diff --git a/radbase/compilation/test_test_1700/Muonic Barrett Moment.json b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json index 5461d2d..81ae28c 100644 --- a/radbase/compilation/test_test_1700/Muonic Barrett Moment.json +++ b/radbase/compilation/test_test_1700/Muonic Barrett Moment.json @@ -1,2619 +1,20 @@ { - "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2": { + "test_test_1700_barrettmoment_Pb203_2p1/2-1s1/2": { "Reference": "test_test_1700", "Previous Muonic Measurements": [ "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2" ], "Nuclide": "Pb203", "Rka [fm]": { - "value": 100.0, - "uncertainty": 3.0 + "Value": 300.0, + "Uncertainty": null }, "k [-]": "1", "alpha [1/fm]": "1", "Cz [fm/keV]": "1", "Nuclear Polarization Method": "Calculated", - "Calculated Nuclear Polarization": [], - "Notes": "" - }, - "test_test_1700_barrettmoment_P32_Pb208-2p1/2-1s1/2_Pb208-2p3/2-1s1/2_Pb208-2s1/2-2p3/2_2s1/2-2p1/2_Pb208-3d3/2-2p1/2_Pb208-3d3/2-2p3/2_Pb208-3d5/2-2p3/2_Pb208-3p1/2-2s1/2_Pb208-3p3/2-2s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3f7/2-3d5/2_3p1/2-2s1/2_3p3/2-2s1/2_4d3/2-3p1/2_4d3/2-3p3/2_4d5/2-3p3/2_4f5/2-3d3/2_4f5/2-3d5/2_5f5/2-3d3/2_5f5/2-3d5/2_5f7/2-3d5/2_NP-Calculated_NP-Fit_Ca40-q=1.010e+00_Ca40-q=1.031e+00_Ca40-q=1.051e+00_Ca40-q=1.071e+00_Ca40-q=1.091e+00_Ca40-q=1.111e+00_Ca40-q=1.150e+00_Ca40-q=1.170e+00_Ca40-q=1.190e+00_Ca40-q=1.228e+00_Ca40-q=1.267e+00_Ca40-q=1.343e+00_Ca40-q=1.400e+00_Ca40-q=1.417e+00_Ca40-q=1.489e+00_Ca40-q=1.520e+00_Ca40-q=1.560e+00_Ca40-q=1.629e+00_Ca40-q=1.650e+00_Ca40-q=1.712e+00_Ca40-q=1.730e+00_Ca40-q=1.792e+00_Ca40-q=1.820e+00_Ca40-q=1.868e+00_Ca40-q=1.900e+00_Ca40-q=1.941e+00_Ca40-q=1.980e+00_Ca40-q=2.010e+00_Ca40-q=2.060e+00_Ca40-q=2.076e+00_Ca40-q=2.137e+00_Ca40-q=2.180e+00_Ca40-q=2.248e+00_Ca40-q=2.300e+00_Ca40-q=2.420e+00_Ca40-q=2.530e+00_Ca40-q=2.650e+00_Ca40-q=6.980e-01_Ca40-q=7.620e-01_Ca40-q=8.140e-01_Ca40-q=8.670e-01_Ca40-q=9.080e-01_Ca40-q=9.490e-01_Ca40-q=9.900e-01_Ca42-q=1.031e+00_Ca42-q=1.071e+00_Ca42-q=1.111e+00_Ca42-q=1.150e+00_Ca42-q=1.190e+00_Ca42-q=1.267e+00_Ca42-q=1.343e+00_Ca42-q=1.417e+00_Ca42-q=1.489e+00_Ca42-q=1.560e+00_Ca42-q=1.629e+00_Ca42-q=1.695e+00_Ca42-q=6.980e-01_Ca42-q=7.830e-01_Ca42-q=8.670e-01_Ca42-q=9.490e-01_Ca44-q=1.031e+00_Ca44-q=1.071e+00_Ca44-q=1.111e+00_Ca44-q=1.150e+00_Ca44-q=1.190e+00_Ca44-q=1.267e+00_Ca44-q=1.343e+00_Ca44-q=1.417e+00_Ca44-q=1.489e+00_Ca44-q=1.560e+00_Ca44-q=1.629e+00_Ca44-q=1.712e+00_Ca44-q=1.792e+00_Ca44-q=6.980e-01_Ca44-q=7.620e-01_Ca44-q=8.140e-01_Ca44-q=8.670e-01_Ca44-q=9.080e-01_Ca44-q=9.490e-01_Ca44-q=9.900e-01_Ca48-q=1.010e+00_Ca48-q=1.031e+00_Ca48-q=1.051e+00_Ca48-q=1.071e+00_Ca48-q=1.091e+00_Ca48-q=1.111e+00_Ca48-q=1.131e+00_Ca48-q=1.150e+00_Ca48-q=1.170e+00_Ca48-q=1.190e+00_Ca48-q=1.228e+00_Ca48-q=1.267e+00_Ca48-q=1.305e+00_Ca48-q=1.343e+00_Ca48-q=1.400e+00_Ca48-q=1.417e+00_Ca48-q=1.489e+00_Ca48-q=1.520e+00_Ca48-q=1.560e+00_Ca48-q=1.629e+00_Ca48-q=1.650e+00_Ca48-q=1.712e+00_Ca48-q=1.730e+00_Ca48-q=1.792e+00_Ca48-q=1.820e+00_Ca48-q=1.868e+00_Ca48-q=1.900e+00_Ca48-q=1.941e+00_Ca48-q=1.980e+00_Ca48-q=2.010e+00_Ca48-q=2.060e+00_Ca48-q=2.076e+00_Ca48-q=2.137e+00_Ca48-q=2.180e+00_Ca48-q=2.248e+00_Ca48-q=2.300e+00_Ca48-q=2.420e+00_Ca48-q=2.530e+00_Ca48-q=6.980e-01_Ca48-q=7.620e-01_Ca48-q=8.140e-01_Ca48-q=8.670e-01_Ca48-q=9.080e-01_Ca48-q=9.490e-01_Ca48-q=9.900e-01_Ti48-q=1.031e+00_Ti48-q=1.071e+00_Ti48-q=1.111e+00_Ti48-q=1.150e+00_Ti48-q=1.190e+00_Ti48-q=1.228e+00_Ti48-q=1.267e+00_Ti48-q=1.305e+00_Ti48-q=1.343e+00_Ti48-q=1.380e+00_Ti48-q=1.417e+00_Ti48-q=1.453e+00_Ti48-q=1.489e+00_Ti48-q=1.525e+00_Ti48-q=1.560e+00_Ti48-q=1.629e+00_Ti48-q=1.712e+00_Ti48-q=1.792e+00_Ti48-q=6.980e-01_Ti48-q=7.620e-01_Ti48-q=8.140e-01_Ti48-q=8.670e-01_Ti48-q=9.080e-01_Ti48-q=9.490e-01_Ti48-q=9.900e-01_fermi-Hg198_fermi-Hg199_fermi-Hg200_fermi-Hg201_fermi-Hg202_fermi-Hg204_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_3d3/2-2p1/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_3d3/2-2p1/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_Hg199-1s1/2_Hg200-1s1/2_Hg201-1s1/2_Hg202-1s1/2_Hg204-1s1/2_Ti48-q=1.003e+00_Ti48-q=1.034e+00_Ti48-q=1.038e+00_Ti48-q=1.063e+00_Ti48-q=1.088e+00_Ti48-q=1.093e+00_Ti48-q=1.122e+00_Ti48-q=1.137e+00_Ti48-q=1.151e+00_Ti48-q=1.180e+00_Ti48-q=1.186e+00_Ti48-q=1.208e+00_Ti48-q=1.235e+00_Ti48-q=1.236e+00_Ti48-q=1.263e+00_Ti48-q=1.283e+00_Ti48-q=1.290e+00_Ti48-q=1.317e+00_Ti48-q=1.331e+00_Ti48-q=1.343e+00_Ti48-q=1.369e+00_Ti48-q=1.378e+00_Ti48-q=1.419e+00_Ti48-q=1.425e+00_Ti48-q=1.472e+00_Ti48-q=1.480e+00_Ti48-q=1.518e+00_Ti48-q=1.537e+00_Ti48-q=1.563e+00_Ti48-q=1.592e+00_Ti48-q=1.609e+00_Ti48-q=1.653e+00_Ti48-q=1.697e+00_Ti48-q=1.741e+00_Ti48-q=1.784e+00_Ti48-q=1.827e+00_Ti48-q=1.869e+00_Ti48-q=1.910e+00_Ti48-q=1.951e+00_Ti48-q=2.031e+00_Ti48-q=2.070e+00_Ti48-q=2.146e+00_Ti48-q=2.220e+00_Ti48-q=2.291e+00_Ti48-q=2.359e+00_Ti48-q=2.424e+00_Ti48-q=5.532e-01_Ti48-q=6.864e-01_Ti48-q=7.680e-01_Ti48-q=8.481e-01_Ti48-q=8.797e-01_Ti48-q=9.111e-01_Ti48-q=9.421e-01_Ti48-q=9.729e-01_Ti48-q=9.883e-01_Ti50-q=1.003e+00_Ti50-q=1.034e+00_Ti50-q=1.038e+00_Ti50-q=1.063e+00_Ti50-q=1.088e+00_Ti50-q=1.093e+00_Ti50-q=1.122e+00_Ti50-q=1.137e+00_Ti50-q=1.151e+00_Ti50-q=1.180e+00_Ti50-q=1.186e+00_Ti50-q=1.208e+00_Ti50-q=1.235e+00_Ti50-q=1.236e+00_Ti50-q=1.263e+00_Ti50-q=1.283e+00_Ti50-q=1.290e+00_Ti50-q=1.317e+00_Ti50-q=1.331e+00_Ti50-q=1.343e+00_Ti50-q=1.369e+00_Ti50-q=1.378e+00_Ti50-q=1.419e+00_Ti50-q=1.425e+00_Ti50-q=1.472e+00_Ti50-q=1.480e+00_Ti50-q=1.518e+00_Ti50-q=1.537e+00_Ti50-q=1.563e+00_Ti50-q=1.592e+00_Ti50-q=1.609e+00_Ti50-q=1.644e+00_Ti50-q=1.653e+00_Ti50-q=1.697e+00_Ti50-q=1.741e+00_Ti50-q=1.784e+00_Ti50-q=1.827e+00_Ti50-q=1.869e+00_Ti50-q=1.910e+00_Ti50-q=1.951e+00_Ti50-q=2.031e+00_Ti50-q=2.070e+00_Ti50-q=2.146e+00_Ti50-q=2.220e+00_Ti50-q=2.291e+00_Ti50-q=2.359e+00_Ti50-q=2.424e+00_Ti50-q=2.487e+00_Ti50-q=5.532e-01_Ti50-q=6.864e-01_Ti50-q=7.680e-01_Ti50-q=8.481e-01_Ti50-q=8.797e-01_Ti50-q=9.111e-01_Ti50-q=9.421e-01_Ti50-q=9.729e-01_Ti50-q=9.883e-01_fermi-Am241_fermi-Am243_fermi-Cd114_fermi-I127_fermi-In115_fermi-Sn116_fermi-Sn124_fermi-Te126_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_fermi-Pb204_fermi-Pb206_fermi-Pb207_fermi-Pb208_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_2s1/2-2p1/2_2s1/2-2p3/2_3d3/2-1s1/2_3d3/2-2p1/2_3d3/2-2p3/2_3d5/2-2p3/2_3p3/2-1s1/2_3p3/2-2s1/2_4f5/2-3d3/2_4f7/2-3d5/2_5f5/2-3d3/2_5f7/2-3d5/2_6f5/2-3d3/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_2p1/2-1s1/2_2s1/2-2p3/2_3d3/2-2p3/2_3d5/2-2p3/2_3d3/2-2p3/2_4f7/2-3d5/2_5f7/2-3d5/2_6f7/2-3d5/2_NP-Calculated_NP-Calculated_NP-Calculated_NP-Calculated_Cr50-q=-1.161e-01_Cr50-q=-1.244e-01_Cr50-q=-1.260e-01_Cr50-q=-1.327e-01_Cr50-q=-1.410e-01_Cr50-q=-1.440e-01_Cr50-q=-1.490e-01_Cr50-q=-1.580e-01_Cr50-q=-1.740e-01_Cr50-q=-1.820e-01_Cr50-q=-1.910e-01_Cr50-q=-1.990e-01_Cr50-q=-2.070e-01_Cr50-q=-2.160e-01_Cr50-q=-2.250e-01_Cr50-q=-2.320e-01_Cr50-q=-2.430e-01_Cr50-q=-2.490e-01_Cr50-q=-2.610e-01_Cr50-q=-2.650e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.530e-01_Cr50-q=2.633e-01_Cr50-q=2.790e-01_Cr50-q=3.040e-01_Cr50-q=3.072e-01_Cr50-q=3.290e-01_Cr50-q=3.494e-01_Cr50-q=3.511e-01_Cr50-q=3.550e-01_Cr50-q=3.793e-01_Cr50-q=3.798e-01_Cr50-q=3.800e-01_Cr50-q=3.950e-01_Cr50-q=4.050e-01_Cr50-q=4.092e-01_Cr50-q=4.310e-01_Cr50-q=4.389e-01_Cr50-q=4.492e-01_Cr50-q=4.828e-01_Cr50-q=4.991e-01_Cr50-q=5.267e-01_Cr50-q=5.490e-01_Cr50-q=5.705e-01_Cr50-q=5.989e-01_Cr50-q=6.144e-01_Cr50-q=6.488e-01_Cr50-q=6.583e-01_Cr50-q=6.987e-01_Cr50-q=7.022e-01_Cr50-q=7.460e-01_Cr50-q=7.486e-01_Cr50-q=7.985e-01_Cr50-q=8.490e-01_Cr50-q=8.983e-01_Cr50-q=9.482e-01_Cr52-q=-1.161e-01_Cr52-q=-1.244e-01_Cr52-q=-1.260e-01_Cr52-q=-1.327e-01_Cr52-q=-1.410e-01_Cr52-q=-1.440e-01_Cr52-q=-1.580e-01_Cr52-q=-1.660e-01_Cr52-q=-1.710e-01_Cr52-q=-1.740e-01_Cr52-q=-1.820e-01_Cr52-q=-1.910e-01_Cr52-q=-1.990e-01_Cr52-q=-2.070e-01_Cr52-q=-2.160e-01_Cr52-q=-2.250e-01_Cr52-q=-2.320e-01_Cr52-q=-2.430e-01_Cr52-q=-2.490e-01_Cr52-q=-2.610e-01_Cr52-q=-2.650e-01_Cr52-q=-2.790e-01_Cr52-q=1.520e-01_Cr52-q=1.774e-01_Cr52-q=2.027e-01_Cr52-q=2.280e-01_Cr52-q=2.530e-01_Cr52-q=2.633e-01_Cr52-q=2.790e-01_Cr52-q=3.040e-01_Cr52-q=3.072e-01_Cr52-q=3.290e-01_Cr52-q=3.494e-01_Cr52-q=3.511e-01_Cr52-q=3.550e-01_Cr52-q=3.793e-01_Cr52-q=3.798e-01_Cr52-q=3.800e-01_Cr52-q=3.950e-01_Cr52-q=4.050e-01_Cr52-q=4.092e-01_Cr52-q=4.310e-01_Cr52-q=4.389e-01_Cr52-q=4.492e-01_Cr52-q=4.828e-01_Cr52-q=4.991e-01_Cr52-q=5.267e-01_Cr52-q=5.490e-01_Cr52-q=5.705e-01_Cr52-q=5.989e-01_Cr52-q=6.144e-01_Cr52-q=6.488e-01_Cr52-q=6.583e-01_Cr52-q=6.987e-01_Cr52-q=7.022e-01_Cr52-q=7.460e-01_Cr52-q=7.486e-01_Cr52-q=7.985e-01_Cr52-q=8.490e-01_Cr52-q=8.983e-01_Cr52-q=9.482e-01_Cr54-q=-1.161e-01_Cr54-q=-1.244e-01_Cr54-q=-1.260e-01_Cr54-q=-1.327e-01_Cr54-q=-1.410e-01_Cr54-q=-1.440e-01_Cr54-q=-1.580e-01_Cr54-q=-1.710e-01_Cr54-q=-1.740e-01_Cr54-q=-1.820e-01_Cr54-q=-1.910e-01_Cr54-q=-1.990e-01_Cr54-q=-2.070e-01_Cr54-q=-2.160e-01_Cr54-q=-2.250e-01_Cr54-q=-2.320e-01_Cr54-q=-2.430e-01_Cr54-q=-2.490e-01_Cr54-q=-2.610e-01_Cr54-q=-2.650e-01_Cr54-q=-2.790e-01_Cr54-q=1.520e-01_Cr54-q=1.774e-01_Cr54-q=2.027e-01_Cr54-q=2.280e-01_Cr54-q=2.530e-01_Cr54-q=2.633e-01_Cr54-q=2.790e-01_Cr54-q=3.040e-01_Cr54-q=3.072e-01_Cr54-q=3.290e-01_Cr54-q=3.494e-01_Cr54-q=3.511e-01_Cr54-q=3.550e-01_Cr54-q=3.793e-01_Cr54-q=3.798e-01_Cr54-q=3.800e-01_Cr54-q=3.950e-01_Cr54-q=4.050e-01_Cr54-q=4.092e-01_Cr54-q=4.310e-01_Cr54-q=4.389e-01_Cr54-q=4.492e-01_Cr54-q=4.828e-01_Cr54-q=4.991e-01_Cr54-q=5.267e-01_Cr54-q=5.490e-01_Cr54-q=5.705e-01_Cr54-q=5.989e-01_Cr54-q=6.144e-01_Cr54-q=6.488e-01_Cr54-q=6.583e-01_Cr54-q=6.987e-01_Cr54-q=7.022e-01_Cr54-q=7.460e-01_Cr54-q=7.486e-01_Cr54-q=7.985e-01_Cr54-q=8.490e-01_Cr54-q=8.983e-01_Cr54-q=9.482e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.534e-01_Cr50-q=2.633e-01_Cr50-q=2.787e-01_Cr50-q=3.041e-01_Cr50-q=3.072e-01_Cr50-q=3.294e-01_Cr50-q=3.511e-01_Cr50-q=3.547e-01_Cr50-q=3.801e-01_Cr50-q=3.950e-01_Cr50-q=4.054e-01_Cr50-q=4.308e-01_Cr50-q=4.389e-01_Cr50-q=4.828e-01_Cr50-q=5.267e-01_Cr50-q=5.705e-01_Cr50-q=6.144e-01_Cr50-q=6.583e-01_Cr50-q=7.022e-01_Cr50-q=7.461e-01_Cr50-q=1.520e-01_Cr50-q=1.774e-01_Cr50-q=2.027e-01_Cr50-q=2.280e-01_Cr50-q=2.534e-01_Cr50-q=2.633e-01_Cr50-q=2.787e-01_Cr50-q=3.041e-01_Cr50-q=3.072e-01_Cr50-q=3.294e-01_Cr50-q=3.511e-01_Cr50-q=3.547e-01_Cr50-q=3.801e-01_Cr50-q=3.950e-01_Cr50-q=4.054e-01_Cr50-q=4.308e-01_Cr50-q=4.389e-01_Cr50-q=4.828e-01_Cr50-q=5.267e-01_Cr50-q=5.705e-01_Cr50-q=6.144e-01_Cr50-q=6.583e-01_Cr50-q=7.022e-01_Cr50-q=7.461e-01_Cr52-q=1.520e-01_Cr52-q=1.774e-01_Cr52-q=2.027e-01_Cr52-q=2.280e-01_Cr52-q=2.534e-01_Cr52-q=2.633e-01_Cr52-q=2.787e-01_Cr52-q=3.041e-01_Cr52-q=3.072e-01_Cr52-q=3.294e-01_Cr52-q=3.511e-01_Cr52-q=3.547e-01_Cr52-q=3.801e-01_Cr52-q=3.950e-01_Cr52-q=4.054e-01_Cr52-q=4.308e-01_Cr52-q=4.389e-01_Cr52-q=4.828e-01_Cr52-q=5.267e-01_Cr52-q=5.705e-01_Cr52-q=6.144e-01_Cr52-q=6.583e-01_Cr52-q=7.022e-01_Cr52-q=7.461e-01_2s1/2-2p3/2_Zr90-1s1/2_NP-Mixed_2p1/2-1s1/2_2p3/2-1s1/2_Sn112-1s1/2_Sn112-2p1/2_Sn112-2p3/2_NP-Calculated_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_Pb104-2p1/2-1s1/2_Pd104-2p1/2-1s1/2_Pd104-2p3/2-1s1/2_Pd104-3d3/2-2p1/2_Pd104-3d5/2-2p3/2_Pd104-4d5/2-2p3/2_Pd104-4f5/2-3d3/2_Pd104-4f7/2-3d5/2_Pd106-2p1/2-1s1/2_Pd106-2p3/2-1s1/2_Pd106-3d3/2-2p1/2_Pd106-3d5/2-2p3/2_Pd106-4d5/2-2p3/2_Pd106-4f5/2-3d3/2_Pd106-4f7/2-3d5/2_Pd108-2p1/2-1s1/2_Pd108-2p3/2-1s1/2_Pd108-3d3/2-2p1/2_Pd108-3d5/2-2p3/2_Pd108-4d5/2-2p3/2_Pd108-4f5/2-3d3/2_Pd108-4f7/2-3d5/2_Pd110-2p1/2-1s1/2_Pd110-2p3/2-1s1/2_Pd110-3d3/2-2p1/2_Pd110-3d5/2-2p3/2_Pd110-4d5/2-2p3/2_Pd110-4f5/2-3d3/2_Pd110-4f7/2-3d5/2_fermi-Pd104_fermi-Pd106_fermi-Pd108_fermi-Pd110_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p1/2-1s1/2_2p3/2-1s1/2_3d3/2-2p1/2_3d5/2-2p3/2_4d5/2-2p3/2_4f5/2-3d3/2_4f7/2-3d5/2_2p-1s_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_(0+,2p3/2)3/2--(0+,1s1/2)1/2+_(2+,2p3/2)1/2--(2+,1s1/2)3/2+_Pb203-2p1/2-1s1/2_(1+,1s1/2)1/2-(2+,1s1/2)1/2_2p1/2-1s1/2_2p3/2-1s1/2_2p3/2-1s1/2_difference-Zr90_Sn112-1s1/2_Sn112-2p1/2_NP-Vary_NP-Calculated_Ca40-2p3/2-1s1/2_Ca42-2p3/2-1s1/2_Ca43-2p3/2-1s1/2_Ca44-2p3/2-1s1/2_Ca46-2p3/2-1s1/2_Ca48-2p3/2-1s1/2_Cr50-2p3/2-1s1/2_Cr52-2p3/2-1s1/2_Cr53-2p3/2-1s1/2_Cr54-2p3/2-1s1/2_Fe56-2p3/2-1s1/2_K39-2p3/2-1s1/2_K41-2p3/2-1s1/2_Mn55-2p3/2-1s1/2_Sc45-2p3/2-1s1/2_Ti46-2p3/2-1s1/2_Ti47-2p3/2-1s1/2_Ti48-2p3/2-1s1/2_Ti49-2p3/2-1s1/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{ - "Reference": "test_test_1700", - "Previous Muonic Measurements": [ - "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2", - "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", - "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", - "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", - "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", - "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", - "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2", - "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2", - "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2", - "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2", - "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2", - "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2", - "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2", - "bergem_nuclear_1988_radius_Pb208_NP_Calculated", - "bergem_nuclear_1988_radius_Pb208_NP_Fit", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.010e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.031e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.051e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.071e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.091e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.111e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.150e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.170e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.190e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.228e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.267e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.343e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.400e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.417e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.489e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.520e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.560e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.629e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.650e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.712e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.730e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.792e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.820e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.868e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.900e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.941e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.980e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.010e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.060e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.076e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.137e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.180e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.248e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.300e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.420e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.530e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.650e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=6.980e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=7.620e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=8.140e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=8.670e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.080e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.490e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.695e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=7.830e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.010e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.051e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.091e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.131e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.170e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.228e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.305e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.400e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.520e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.650e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.730e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.820e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.868e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.900e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.941e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.980e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.010e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.060e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.076e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.137e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.180e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.248e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.300e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.420e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.530e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.228e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.305e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.380e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.453e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.525e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.900e-01", - "hahn_experimental_1979_fermi_Hg198", - "hahn_experimental_1979_fermi_Hg199", - "hahn_experimental_1979_fermi_Hg200", - "hahn_experimental_1979_fermi_Hg201", - "hahn_experimental_1979_fermi_Hg202", - "hahn_experimental_1979_fermi_Hg204", - "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg198_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg198_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg200_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg200_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg202_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg202_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg204_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg204_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg199_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg200_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg201_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg202_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg204_1s1/2", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.003e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.034e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.038e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.063e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.088e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.093e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.122e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.137e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.151e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.180e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.186e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.208e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.235e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.236e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.263e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.283e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.290e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.317e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.331e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.343e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.369e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.378e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.419e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.425e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.472e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.480e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.518e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.537e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.563e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.592e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.609e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.653e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.697e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.741e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.784e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.827e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.869e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.910e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.951e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.031e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.070e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.146e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.220e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.291e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.359e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.424e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=5.532e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=6.864e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=7.680e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.481e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.797e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.111e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.421e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.729e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.883e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.003e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.034e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.038e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.063e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.088e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.093e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.122e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.137e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.151e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.180e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.186e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.208e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.235e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.236e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.263e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.283e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.290e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.317e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.331e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.343e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.369e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.378e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.419e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.425e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.472e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.480e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.518e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.537e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.563e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.592e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.609e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.644e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.653e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.697e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.741e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.784e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.827e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.869e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.910e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.951e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.031e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.070e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.146e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.220e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.291e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.359e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.424e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.487e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=5.532e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=6.864e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=7.680e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.481e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.797e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.111e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.421e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.729e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.883e-01", - "johnson_241am_1985_fermi_Am241", - "johnson_241am_1985_fermi_Am243", - "kast_isotone_1971_fermi_Cd114", - "kast_isotone_1971_fermi_I127", - "kast_isotone_1971_fermi_In115", - "kast_isotone_1971_fermi_Sn116", - "kast_isotone_1971_fermi_Sn124", - "kast_isotone_1971_fermi_Te126", - "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", - "kast_isotone_1971_muonic_I127_2p1/2_1s1/2", - "kast_isotone_1971_muonic_I127_2p3/2_1s1/2", - "kast_isotone_1971_muonic_I127_3d3/2_2p1/2", - "kast_isotone_1971_muonic_I127_3d5/2_2p3/2", - "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", - "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", - "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", - "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2", - "kast_isotone_1971_radius_Cd114_NP_Calculated", - "kast_isotone_1971_radius_I127_NP_Calculated", - "kast_isotone_1971_radius_In115_NP_Calculated", - "kast_isotone_1971_radius_Sn116_NP_Calculated", - "kast_isotone_1971_radius_Sn124_NP_Calculated", - "kast_isotone_1971_radius_Te126_NP_Calculated", - "kessler_muonic_1975_fermi_Pb204", - "kessler_muonic_1975_fermi_Pb206", - "kessler_muonic_1975_fermi_Pb207", - "kessler_muonic_1975_fermi_Pb208", - "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_radius_Pb204_NP_Calculated", - "kessler_muonic_1975_radius_Pb206_NP_Calculated", - "kessler_muonic_1975_radius_Pb207_NP_Calculated", - "kessler_muonic_1975_radius_Pb208_NP_Calculated", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.660e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.710e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.710e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.461e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.461e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.461e-01", - "phan_nuclear_1985_muonic_Zr90_2s1/2_2p3/2", - "phan_nuclear_1985_muonic_nuclear_polarization_Zr90_1s1/2", - "phan_nuclear_1985_radius_Zr90_NP_Mixed", - "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2", - "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2", - "piller_nuclear_1990_radius_Sn112_NP_Calculated", - "powers_hyperfine_1968_muonic_Bi209_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_2p1/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_3d3/2_2p1/2", - "powers_hyperfine_1968_muonic_Pb206_3d5/2_2p3/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p1/2_1s1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d3/2_2p1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d5/2_2p3/2", - "saito_muonic_2025_barrett_moment_Pb104_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd104_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd104_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd104_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd104_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd106_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd106_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd106_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd106_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd106_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd106_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd106_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd108_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd108_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd108_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd108_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd108_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd108_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd108_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd110_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd110_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd110_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd110_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd110_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd110_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd110_4f7/2-3d5/2", - "saito_muonic_2025_fermi_Pd104", - "saito_muonic_2025_fermi_Pd106", - "saito_muonic_2025_fermi_Pd108", - "saito_muonic_2025_fermi_Pd110", - "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2", - "schaller_nuclear_1985_muonic_P31_2p_1s", - "shera_systematics_1976_muonic_Co59_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe54_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe56_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe57_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe58_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni58_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni60_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe56_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe56_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe57_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn70_2p3/2_1s1/2", - "tanaka_measurement_1984_muonic_Hf176_(0+,2p3/2)3/2-_(0+,1s1/2)1/2+", - "tanaka_measurement_1984_muonic_Hf176_(2+,2p3/2)1/2-_(2+,1s1/2)3/2+", - "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2", - "test_test_1700_muonic_Pb203_(1+,1s1/2)1/2_(2+,1s1/2)1/2", - "test_test_1700_muonic_Sn112_2p1/2_1s1/2", - "test_test_1700_muonic_difference_Fe1_Fe3_2p3/2_1s1/2", - "test_test_1700_muonic_difference_Fe2_Fe4_2p3/2_1s1/2", - "test_test_1700_muonic_difference_Zr90", - "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", - "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2", - "test_test_1700_radius_Pb203_NP_Vary", - "test_test_1700_radius_Pb204_NP_Calculated", - "wolfhahrt_nuclear_1981_barrett_moment_Ca40_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca42_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca43_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca44_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca46_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca48_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr50_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr52_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr53_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr54_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Fe56_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_K39_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_K41_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Mn55_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Sc45_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti46_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti47_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti48_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti49_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti50_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_V51_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_fermi_Ca40", - "wolfhahrt_nuclear_1981_fermi_Ca42", - "wolfhahrt_nuclear_1981_fermi_Ca43", - "wolfhahrt_nuclear_1981_fermi_Ca44", - "wolfhahrt_nuclear_1981_fermi_Ca46", - "wolfhahrt_nuclear_1981_fermi_Ca48", - "wolfhahrt_nuclear_1981_fermi_Cr50", - "wolfhahrt_nuclear_1981_fermi_Cr52", - "wolfhahrt_nuclear_1981_fermi_Cr53", - "wolfhahrt_nuclear_1981_fermi_Cr54", - "wolfhahrt_nuclear_1981_fermi_Fe56", - "wolfhahrt_nuclear_1981_fermi_K39", - "wolfhahrt_nuclear_1981_fermi_K41", - "wolfhahrt_nuclear_1981_fermi_Mn55", - "wolfhahrt_nuclear_1981_fermi_Sc45", - "wolfhahrt_nuclear_1981_fermi_Ti46", - "wolfhahrt_nuclear_1981_fermi_Ti47", - "wolfhahrt_nuclear_1981_fermi_Ti48", - "wolfhahrt_nuclear_1981_fermi_Ti49", - "wolfhahrt_nuclear_1981_fermi_Ti50", - "wolfhahrt_nuclear_1981_fermi_V51", - "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_K41_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" - ], - "Nuclide": "P32", - "Rka [fm]": { - "Value": 0.0, - "Uncertainty": null - }, - "k [-]": "0", - "alpha [1/fm]": "0", - "Cz [fm/keV]": "0", - "Nuclear Polarization Method": "Calculated", "Calculated Nuclear Polarization": [ - "bergem_nuclear_1988_barrett_moment_Pb208_2p1/2-1s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2p3/2-1s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_2s1/2_2p1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d3/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3d5/2-2p3/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3p1/2-2s1/2", - "bergem_nuclear_1988_barrett_moment_Pb208_3p3/2-2s1/2", - "bergem_nuclear_1988_muonic_Pb208_2p1/2_1s1/2", - "bergem_nuclear_1988_muonic_Pb208_2p3/2_1s1/2", - "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p1/2", - "bergem_nuclear_1988_muonic_Pb208_2s1/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p1/2", - "bergem_nuclear_1988_muonic_Pb208_3d3/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3d5/2_2p3/2", - "bergem_nuclear_1988_muonic_Pb208_3f7/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_3p1/2_2s1/2", - "bergem_nuclear_1988_muonic_Pb208_3p3/2_2s1/2", - "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p1/2", - "bergem_nuclear_1988_muonic_Pb208_4d3/2_3p3/2", - "bergem_nuclear_1988_muonic_Pb208_4d5/2_3p3/2", - "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d3/2", - "bergem_nuclear_1988_muonic_Pb208_4f5/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d3/2", - "bergem_nuclear_1988_muonic_Pb208_5f5/2_3d5/2", - "bergem_nuclear_1988_muonic_Pb208_5f7/2_3d5/2", - "bergem_nuclear_1988_radius_Pb208_NP_Calculated", - "bergem_nuclear_1988_radius_Pb208_NP_Fit", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.010e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.031e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.051e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.071e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.091e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.111e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.150e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.170e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.190e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.228e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.267e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.343e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.400e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.417e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.489e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.520e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.560e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.629e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.650e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.712e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.730e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.792e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.820e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.868e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.900e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.941e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=1.980e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.010e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.060e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.076e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.137e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.180e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.248e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.300e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.420e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.530e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=2.650e+00", - "frosch_electron_1968_electroncrosssection_Ca40_q=6.980e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=7.620e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=8.140e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=8.670e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.080e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.490e-01", - "frosch_electron_1968_electroncrosssection_Ca40_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=1.695e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=7.830e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca42_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca44_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.010e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.051e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.091e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.131e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.170e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.228e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.305e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.400e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.520e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.650e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.730e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.820e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.868e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.900e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.941e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=1.980e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.010e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.060e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.076e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.137e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.180e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.248e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.300e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.420e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=2.530e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca40_Ca48_q=9.900e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.031e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.071e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.111e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.150e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.190e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.228e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.267e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.305e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.343e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.380e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.417e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.453e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.489e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.525e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.560e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.629e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.712e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=1.792e+00", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=6.980e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=7.620e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.140e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=8.670e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.080e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.490e-01", - "frosch_electron_1968_electroncrosssectionratio_Ca48_Ti48_q=9.900e-01", - "hahn_experimental_1979_fermi_Hg198", - "hahn_experimental_1979_fermi_Hg199", - "hahn_experimental_1979_fermi_Hg200", - "hahn_experimental_1979_fermi_Hg201", - "hahn_experimental_1979_fermi_Hg202", - "hahn_experimental_1979_fermi_Hg204", - "hahn_experimental_1979_muonic_Hg198_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg198_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg198_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg198_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg198_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg198_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg199_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg199_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg199_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg200_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg200_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg200_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg200_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg200_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg200_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg201_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg201_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg201_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg202_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg202_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg202_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg202_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg202_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg202_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_Hg204_2p1/2_1s1/2", - "hahn_experimental_1979_muonic_Hg204_2p3/2_1s1/2", - "hahn_experimental_1979_muonic_Hg204_3d3/2_2p1/2", - "hahn_experimental_1979_muonic_Hg204_3d5/2_2p3/2", - "hahn_experimental_1979_muonic_Hg204_4f5/2_3d3/2", - "hahn_experimental_1979_muonic_Hg204_4f7/2_3d5/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg199_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg200_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg201_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg202_1s1/2", - "hahn_experimental_1979_muonic_difference_Hg198_Hg204_1s1/2", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.003e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.034e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.038e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.063e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.088e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.093e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.122e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.137e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.151e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.180e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.186e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.208e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.235e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.236e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.263e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.283e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.290e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.317e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.331e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.343e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.369e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.378e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.419e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.425e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.472e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.480e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.518e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.537e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.563e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.592e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.609e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.653e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.697e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.741e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.784e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.827e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.869e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.910e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=1.951e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.031e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.070e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.146e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.220e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.291e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.359e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=2.424e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=5.532e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=6.864e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=7.680e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.481e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=8.797e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.111e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.421e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.729e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti46_Ti48_q=9.883e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.003e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.034e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.038e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.063e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.088e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.093e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.122e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.137e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.151e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.180e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.186e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.208e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.235e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.236e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.263e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.283e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.290e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.317e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.331e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.343e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.369e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.378e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.419e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.425e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.472e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.480e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.518e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.537e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.563e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.592e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.609e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.644e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.653e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.697e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.741e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.784e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.827e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.869e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.910e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=1.951e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.031e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.070e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.146e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.220e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.291e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.359e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.424e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=2.487e+00", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=5.532e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=6.864e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=7.680e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.481e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=8.797e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.111e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.421e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.729e-01", - "heisenberg_electron_1972_electroncrosssectionratio_Ti48_Ti50_q=9.883e-01", - "johnson_241am_1985_fermi_Am241", - "johnson_241am_1985_fermi_Am243", - "kast_isotone_1971_fermi_Cd114", - "kast_isotone_1971_fermi_I127", - "kast_isotone_1971_fermi_In115", - "kast_isotone_1971_fermi_Sn116", - "kast_isotone_1971_fermi_Sn124", - "kast_isotone_1971_fermi_Te126", - "kast_isotone_1971_muonic_Cd114_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Cd114_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Cd114_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Cd114_3d5/2_2p3/2", - "kast_isotone_1971_muonic_I127_2p1/2_1s1/2", - "kast_isotone_1971_muonic_I127_2p3/2_1s1/2", - "kast_isotone_1971_muonic_I127_3d3/2_2p1/2", - "kast_isotone_1971_muonic_I127_3d5/2_2p3/2", - "kast_isotone_1971_muonic_In115_2p1/2_1s1/2", - "kast_isotone_1971_muonic_In115_2p3/2_1s1/2", - "kast_isotone_1971_muonic_In115_3d3/2_2p1/2", - "kast_isotone_1971_muonic_In115_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Sn116_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Sn116_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Sn116_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Sn116_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Sn124_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Sn124_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Sn124_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Sn124_3d5/2_2p3/2", - "kast_isotone_1971_muonic_Te126_2p1/2_1s1/2", - "kast_isotone_1971_muonic_Te126_2p3/2_1s1/2", - "kast_isotone_1971_muonic_Te126_3d3/2_2p1/2", - "kast_isotone_1971_muonic_Te126_3d5/2_2p3/2", - "kast_isotone_1971_radius_Cd114_NP_Calculated", - "kast_isotone_1971_radius_I127_NP_Calculated", - "kast_isotone_1971_radius_In115_NP_Calculated", - "kast_isotone_1971_radius_Sn116_NP_Calculated", - "kast_isotone_1971_radius_Sn124_NP_Calculated", - "kast_isotone_1971_radius_Te126_NP_Calculated", - "kessler_muonic_1975_fermi_Pb204", - "kessler_muonic_1975_fermi_Pb206", - "kessler_muonic_1975_fermi_Pb207", - "kessler_muonic_1975_fermi_Pb208", - "kessler_muonic_1975_muonic_Pb204_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb204_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb204_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb204_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb204_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb204_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb204_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb204_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb204_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb206_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb206_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb206_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb206_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb206_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb206_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb206_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb207_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb207_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb207_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb207_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb207_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb207_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb207_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_2p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_2s1/2_2p1/2", - "kessler_muonic_1975_muonic_Pb208_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_2p1/2", - "kessler_muonic_1975_muonic_Pb208_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_Pb208_3p3/2_1s1/2", - "kessler_muonic_1975_muonic_Pb208_3p3/2_2s1/2", - "kessler_muonic_1975_muonic_Pb208_4f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_5f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_Pb208_6f5/2_3d3/2", - "kessler_muonic_1975_muonic_Pb208_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb204_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb206_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb207_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_2p3/2_1s1/2_B_2p1/2_1s1/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_2s1/2_2p1/2_B_2s1/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d3/2_2p1/2_B_3d5/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_3d5/2_2p3/2_B_3d3/2_2p3/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_4f5/2_3d3/2_B_4f5/2_4f7/2_C_4f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_5f5/2_3d3/2_B_5f5/2_5f7/2_C_5f7/2_3d5/2", - "kessler_muonic_1975_muonic_difference_Pb208_A_6f5/2_3d3/2_B_6f5/2_6f7/2_C_6f7/2_3d5/2", - "kessler_muonic_1975_radius_Pb204_NP_Calculated", - "kessler_muonic_1975_radius_Pb206_NP_Calculated", - "kessler_muonic_1975_radius_Pb207_NP_Calculated", - "kessler_muonic_1975_radius_Pb208_NP_Calculated", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr50_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.660e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.710e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=-2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr52_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.161e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.244e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.260e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.327e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.410e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.440e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.580e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.710e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.740e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.820e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.910e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-1.990e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.070e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.160e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.250e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.320e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.430e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.610e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.650e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=-2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.530e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=2.790e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.040e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.290e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.494e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.550e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.793e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.798e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.800e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.050e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.092e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.310e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.492e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=4.991e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=5.989e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.488e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=6.987e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.460e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.486e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=7.985e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.490e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=8.983e-01", - "lightbody_elastic_1983_electroncrosssection_Cr54_q=9.482e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr52_Cr50_q=7.461e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr50_q=7.461e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.520e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=1.774e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.027e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.280e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.534e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.633e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=2.787e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.041e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.072e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.294e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.511e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.547e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.801e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=3.950e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.054e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.308e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.389e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=4.828e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.267e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=5.705e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.144e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=6.583e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.022e-01", - "lightbody_elastic_1983_electroncrosssectionratio_Cr54_Cr52_q=7.461e-01", - "phan_nuclear_1985_muonic_Zr90_2s1/2_2p3/2", - "phan_nuclear_1985_muonic_nuclear_polarization_Zr90_1s1/2", - "phan_nuclear_1985_radius_Zr90_NP_Mixed", - "piller_nuclear_1990_muonic_Sn112_2p1/2_1s1/2", - "piller_nuclear_1990_muonic_Sn112_2p3/2_1s1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_1s1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2", - "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p3/2", - "piller_nuclear_1990_radius_Sn112_NP_Calculated", - "powers_hyperfine_1968_muonic_Bi209_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_2p1/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_Pb206_3d3/2_2p1/2", - "powers_hyperfine_1968_muonic_Pb206_3d5/2_2p3/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p1/2_1s1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_2p3/2_1s1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d3/2_2p1/2", - "powers_hyperfine_1968_muonic_difference_Bi209_Pb206_3d5/2_2p3/2", - "saito_muonic_2025_barrett_moment_Pb104_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd104_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd104_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd104_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd104_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd104_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd106_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd106_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd106_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd106_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd106_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd106_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd106_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd108_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd108_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd108_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd108_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd108_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd108_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd108_4f7/2-3d5/2", - "saito_muonic_2025_barrett_moment_Pd110_2p1/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd110_2p3/2-1s1/2", - "saito_muonic_2025_barrett_moment_Pd110_3d3/2-2p1/2", - "saito_muonic_2025_barrett_moment_Pd110_3d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd110_4d5/2-2p3/2", - "saito_muonic_2025_barrett_moment_Pd110_4f5/2-3d3/2", - "saito_muonic_2025_barrett_moment_Pd110_4f7/2-3d5/2", - "saito_muonic_2025_fermi_Pd104", - "saito_muonic_2025_fermi_Pd106", - "saito_muonic_2025_fermi_Pd108", - "saito_muonic_2025_fermi_Pd110", - "saito_muonic_2025_muonic_Pd104_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd104_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd104_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd104_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd104_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd104_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd104_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd106_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd106_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd106_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd106_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd106_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd106_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd106_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd108_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd108_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd108_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd108_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd108_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd108_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd108_4f7/2_3d5/2", - "saito_muonic_2025_muonic_Pd110_2p1/2_1s1/2", - "saito_muonic_2025_muonic_Pd110_2p3/2_1s1/2", - "saito_muonic_2025_muonic_Pd110_3d3/2_2p1/2", - "saito_muonic_2025_muonic_Pd110_3d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd110_4d5/2_2p3/2", - "saito_muonic_2025_muonic_Pd110_4f5/2_3d3/2", - "saito_muonic_2025_muonic_Pd110_4f7/2_3d5/2", - "schaller_nuclear_1985_muonic_P31_2p_1s", - "shera_systematics_1976_muonic_Co59_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe54_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe56_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe57_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Fe58_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni58_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni60_2p1/2_1s1/2", - "shera_systematics_1976_muonic_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Co59_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu63_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Cu65_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe54_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe56_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe56_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Fe57_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni58_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni60_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni61_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni62_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Ni64_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn64_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn66_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn68_Zn70_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_difference_Zn70_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Co59_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Cu63_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Cu65_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe54_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe57_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Fe58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni58_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni60_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni61_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni62_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Ni64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn64_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn66_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn68_2p3/2_1s1/2", - "shera_systematics_1976_muonic_nuclear_polarization_Zn70_2p3/2_1s1/2", - "tanaka_measurement_1984_muonic_Hf176_(0+,2p3/2)3/2-_(0+,1s1/2)1/2+", - "tanaka_measurement_1984_muonic_Hf176_(2+,2p3/2)1/2-_(2+,1s1/2)3/2+", - "test_test_1700_barrett_moment_Pb203_2p1/2-1s1/2", - "test_test_1700_muonic_Pb203_(1+,1s1/2)1/2_(2+,1s1/2)1/2", - "test_test_1700_muonic_Sn112_2p1/2_1s1/2", - "test_test_1700_muonic_difference_Fe1_Fe3_2p3/2_1s1/2", - "test_test_1700_muonic_difference_Fe2_Fe4_2p3/2_1s1/2", - "test_test_1700_muonic_difference_Zr90", - "test_test_1700_muonic_nuclear_polarization_Sn112_1s1/2", - "test_test_1700_muonic_nuclear_polarization_Sn112_2p1/2", - "test_test_1700_radius_Pb203_NP_Vary", - "test_test_1700_radius_Pb204_NP_Calculated", - "wolfhahrt_nuclear_1981_barrett_moment_Ca40_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca42_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca43_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca44_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca46_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ca48_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr50_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr52_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr53_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Cr54_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Fe56_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_K39_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_K41_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Mn55_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Sc45_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti46_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti47_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti48_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti49_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_Ti50_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_barrett_moment_V51_2p3/2-1s1/2", - "wolfhahrt_nuclear_1981_fermi_Ca40", - "wolfhahrt_nuclear_1981_fermi_Ca42", - "wolfhahrt_nuclear_1981_fermi_Ca43", - "wolfhahrt_nuclear_1981_fermi_Ca44", - "wolfhahrt_nuclear_1981_fermi_Ca46", - "wolfhahrt_nuclear_1981_fermi_Ca48", - "wolfhahrt_nuclear_1981_fermi_Cr50", - "wolfhahrt_nuclear_1981_fermi_Cr52", - "wolfhahrt_nuclear_1981_fermi_Cr53", - "wolfhahrt_nuclear_1981_fermi_Cr54", - "wolfhahrt_nuclear_1981_fermi_Fe56", - "wolfhahrt_nuclear_1981_fermi_K39", - "wolfhahrt_nuclear_1981_fermi_K41", - "wolfhahrt_nuclear_1981_fermi_Mn55", - "wolfhahrt_nuclear_1981_fermi_Sc45", - "wolfhahrt_nuclear_1981_fermi_Ti46", - "wolfhahrt_nuclear_1981_fermi_Ti47", - "wolfhahrt_nuclear_1981_fermi_Ti48", - "wolfhahrt_nuclear_1981_fermi_Ti49", - "wolfhahrt_nuclear_1981_fermi_Ti50", - "wolfhahrt_nuclear_1981_fermi_V51", - "wolfhahrt_nuclear_1981_muonic_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca40_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca42_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca43_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca44_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca46_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ca48_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr50_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr52_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr53_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Cr54_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Fe56_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_K41_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Mn55_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Sc45_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti46_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti47_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti48_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti49_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_Ti50_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_difference_V51_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_nuclear_polarization_V51_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca40_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca42_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca43_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca44_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ca48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr52_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr53_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Cr54_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Fe56_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_K39_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_K41_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Mn55_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Sc45_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti46_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti47_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti48_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti49_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_Ti50_2p3/2_1s1/2", - "wolfhahrt_nuclear_1981_muonic_qed_V51_2p3/2_1s1/2" + "piller_nuclear_1990_muonic_nuclear_polarization_Sn112_2p1/2" ], "Notes": "" } diff --git a/radbase/data_entry.py b/radbase/data_entry.py index e8bc2a0..923c6cf 100644 --- a/radbase/data_entry.py +++ b/radbase/data_entry.py @@ -337,7 +337,7 @@ def process(self, widget: tk.Widget) -> dict[str, list[str]]: @staticmethod def unpack_widget(widget: tk.Widget): - return {key: checkbox for key, checkbox in widget.selection_vars.items()} + return {key: checkbox.get() for key, checkbox in widget.selection_vars.items()} def process_data(self, data: dict) -> dict[str, list[str]]: selected = [key for key, var in data.items() if var] diff --git a/tests/test_data_entry.py b/tests/test_data_entry.py index c07edbb..e31b8e3 100644 --- a/tests/test_data_entry.py +++ b/tests/test_data_entry.py @@ -105,8 +105,11 @@ def test_reference_processor(tmp_path): def test_previous_data_processor(tmp_path): - options = {'test_test_0000_data1': True, - 'test_test_0000_data2': False} + true_widget = DummyWidget(True) + false_widget = DummyWidget(False) + + options = {'test_test_0000_data1': true_widget, + 'test_test_0000_data2': false_widget} previous_widget = DummyWidget('') previous_widget.selection_vars = options