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/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 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"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 new file mode 100644 index 0000000..b67bb50 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections.csv @@ -0,0 +1,165 @@ +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 +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 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+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..86f052e --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_a.csv @@ -0,0 +1,42 @@ +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 +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..ac53c19 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_b.csv @@ -0,0 +1,31 @@ +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±1.1ᶜ +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 +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..0441277 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/cross_sections_c.csv @@ -0,0 +1,15 @@ +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 +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..273e779 --- /dev/null +++ b/radbase/compilation/frosch_electron_1968/frosch_1968_process.py @@ -0,0 +1,104 @@ +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') + +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(['', '...',]) | df[column].isna())] + 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) + +interface = DataEntryInterface(start_interface=False) + +for i, row in by_quant_dfs.iterrows(): + + 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/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]": { 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}, + "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/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, + 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"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/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": 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+ "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/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 new file mode 100644 index 0000000..3456ab5 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/Muonic Transition Energy Difference (different nuclides).json @@ -0,0 +1,2942 @@ +{ + "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/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 new file mode 100644 index 0000000..1a7a32a --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/energy_diffs.csv @@ -0,0 +1,210 @@ +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..9f14bd1 --- /dev/null +++ b/radbase/compilation/wolfhahrt_nuclear_1981/wolfhart_1981_process.py @@ -0,0 +1,126 @@ +import csv + +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', + '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. ' +} + +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', + 'a [fm]': {'Value': 0.55, + 'Uncertainty': None}, + 'Notes': 'a fixed, c varied to reproduce 2p3/2-1s1/2 energies.' +} + +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') + +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 f49a698..d88fe40 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) @@ -103,7 +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 @@ -114,31 +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 @@ -149,15 +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 @@ -176,29 +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')] @@ -206,15 +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]') @@ -225,10 +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 @@ -249,10 +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]{2}\d{1,3}', raw) or re.match(r'[a-zA-Z]{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') @@ -263,9 +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} @@ -285,15 +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)) + + @staticmethod + def unpack_widget(widget: tk.Widget) -> str: + return widget.get().strip() - if value not in sorted(self.references.keys()): + 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: @@ -341,8 +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") @@ -529,7 +616,7 @@ 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 +642,7 @@ 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 @@ -929,13 +1016,14 @@ 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 +1031,11 @@ 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 +1043,8 @@ 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()], ()))]) ) @@ -976,11 +1069,32 @@ 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=[ 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 +1113,34 @@ 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")?'), + FieldSpec('QED Calculations Used', + PreviousDataProcessor(key='Calculated QED'), + PreviousDataWidgetCreator(compilation_path=config['compilation_dir'])), + 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=[ @@ -1037,13 +1179,48 @@ 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, muonic_nuclear_polarization_calculation_template, + muonic_qed_calculation_template, 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: @@ -1081,7 +1258,7 @@ 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): @@ -1163,6 +1340,7 @@ 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, @@ -1463,7 +1641,7 @@ 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: