ADOPTED LEVELS, GAMMAS for 56Ca
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 08-Sep-2023
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 25-Mar-2022
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 31-OCT-2011
Author: Balraj Singh | Citation: ENSDF | Cutoff date: 10-MAY-2009
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=1201×101 keV 36 | S(n)= 293×101 keV 30 | S(p)= 21270 keV SY | Q(α)= -14560 keV SY | ||
Reference: 2021WA16 |
References: | |||
A | 1H(57Sc,2pγ) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) |
0 | A | 0+ | 11 ms 2 % β- = 100 % β-n = ? % β-2n = ? % B-3N = ? | ||
1456 12 | A | (2+) | 1456 12 | 100 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 0+ | 11 ms 2 % β- = 100 % β-n = ? % β-2n = ? % B-3N = ? | Theoretical T1/2=24.2 ms, %β-n=8, %β-2n=0, %β-3n=0 (2019Mo01). E(level): Theoretical T1/2=24.2 ms, %β-n=8, %β-2n=0, %β-3n=0 (2019Mo01). |
1456 | (2+) | Measured partial cross section for the 1456,(2+) level=0.43 mb 4 (2023Ch26). |
E(level) | E(gamma) | Comments |
1456 | 1456 | E(γ): from 1H(57Sc,2pγ) |
1997Be70: 56Ca identified in 9Be(238U,F), E=750 MeV/nucleon, fragments separator (FRS) at GSI facility, identification by time-of-flight. Measured production cross section
2008Ma01: 56Ca isotope produced in 9Be(76Ge,X) reaction at E=140 MeV/nucleon 76Ge beam provided by NSCL at Michigan State University. Isotopes separated with A1900 fragment separator. Time-of-flight technique. Measured β particles using Beta Counting System of three Si PIN detectors, a double-sided silicon strip detector and six single sided silicon strip detectors. Detected γ rays using 16 Ge detectors of the Segmented Germanium array. Measured half-life of 56Ca by fitting the decay curves to a function which included decay of the parent, growth and decay of daughter and a constant background. No gamma rays were seen in correlation with β rays.
2018Mi08: measured mass excess
Theoretical structure calculations:
2023Kr01: calculated the nuclear ground state using relativistic Hartree-Bogoliubov model, and the M2 excitations using the relativistic QRPA with residual interaction.
2022Co05: calculated binding energies, isotope shifts, charge radii using independent particle model based on Hartree-Fock plus Bardeen-Cooper-Schrieffer (HF+BCS) approach.
2022Ko04: calculated ground state energies, charge rms radii using coupled cluster (α) and ab-initio density functional theory.
2022Ku16: calculated potential energy surfaces, binding energy, S(2n), charge radius, neutron and proton rms radii, neutron skin thickness using covariant density functional theory with several Skyrme parametrizations.
2021Fu11: calculated energy levels, Jπ, S(2n) using realistic shell model with chiral interaction.
2021Ma73: calculated levels, Jπ, S(2n), two-body matrix elements (TBME) using state-of-the-art in-medium similarity renormalization group (IMSRG) interaction, with universal fp shell interaction.
2020Bh06: calculated energy levels, Jπ, occupancy, B(E2), nuclear magnetic moments, spectroscopic factors, wave functions using shell model in several model spaces.
2020Co10: calculated energy of the first 2+ state, S(2n) using shell model.
2020Li35: calculated binding energy, S(n), S(2n), neutron effective single-particle energies (ESPE), levels, Jπ using realistic Gamow shell model
2012Ha26: calculated ground state energy, Jπ using chiral effective field theory.
2009Co19: calculated levels, Jπ, neutron-neutron two-body matrix elements using shell-model with a realistic effective interaction from the Cd-Bonn nucleon-nucleon potential.
1998Br30: calculated binding energy, levels, Jπ using shell model plus Hartree-Fock approach.
Other theoretical structure calculations: 105 primary reference extracted from the NSR database are listed under ’document’ records in this dataset.
Q-value: Estimated uncertainties (2021Wa16): 560 for S(p), 650 for Q(α)
Q-value: Q(β-n)=9260 260, S(2n)=4490 250, S(2p)=40650 840 (syst) (2021Wa16).
Q-value: Q(β-2n)=4785 250, Q(β-3n)=1046 250 deduced by evaluator from relevant mass excesses in 2021Wa16