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MOCCA/examples/fe_stat_n15.json
2026-04-19 19:42:30 +02:00

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{
"schema_version": 1,
"metadata": {
"case_name": "fe_stat_n15"
},
"atom": {
"atomic_number": 26.0,
"effective_shell_charges": [24.0, 22.0, 17.0],
"binding_energies_ev": [7.112e3, 8.46e2, 7.6e1],
"atomic_mass": 56.0,
"exact_mass_number": null
},
"masses": {
"muon_electron_masses": 206.7686,
"electron_mass_ev": 511003.4,
"nucleon_mass_mev": 931.48
},
"transitions": {
"two_p_to_one_s_energy_ev": null,
"two_s_to_two_p_split_ev": null,
"dirac_energies": []
},
"capture": {
"mode": "statistical_l",
"n_max": 15,
"alpha": 0.22
},
"channels": {
"case_counts": [3, 4, 4, 4],
"monopole_shells": [1, 2, 3],
"dipole_shells": [0, 1, 2, 3],
"quadrupole_shells": [0, 1, 2, 3],
"octupole_shells": [0, 1, 2, 3],
"dipole_subshell_channels": [0, 0, 0, 0],
"quadrupole_subshell_channels": [0, 0, 0, 0],
"octupole_subshell_channels": [0, 0, 0, 0],
"dipole_penetration_codes": [0, 1, 1, 1],
"quadrupole_penetration_codes": [0, 1, 1, 1],
"octupole_penetration_codes": [0, 1, 1, 1],
"dipole_penetration_avg_n_cutoffs": [0, 0, 0, 0],
"quadrupole_penetration_avg_n_cutoffs": [0, 0, 0, 0],
"octupole_penetration_avg_n_cutoffs": [0, 0, 0, 0]
},
"shell_model": {
"subshell_populations": [1, 1, 1, 1, 1, 1],
"refill_codes": [0, 0, 0],
"penetration_cutoffs": [1, 1, 1, 1],
"width_k_ev": 0.0,
"track_polarization": true
},
"reporting": {
"line_energy_min_mev": 0.04,
"line_energy_max_mev": 20.0,
"line_intensity_threshold": 1.0e-6,
"energy_resolution_mev": 0.0003
},
"model": {
"factorial_divider": 15.0
},
"numerics": {
"matrix_element_precision_digits": 120
}
}