beta(-) decay of neutron-rich Cl-45 located at the magic number N=28

Soumik Bhattacharya,Vandana Tripathi, S. L. Tabor, A. Volya, P. C. Bender, C. Benetti,M. P. Carpenter,J. J. Carroll,A. Chester, C. J. Chiara, K. Childers,B. R. Clark, B. P. Crider, J. T. Harke,R. Jain,S. N. Liddick, R. S. Lubna, S. Luitel, B. Longfellow, M. J. Mogannam, T. H. Ogunbeku, J. Perello, A. L. Richard, E. Rubino, S. Saha, O. A. Shehu, R. Unz, Y. Xiao,Yiyi Zhu

PHYSICAL REVIEW C(2023)

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摘要
Results from the study of the beta(-) decay of Cl-45, produced in the fragmentation of a 140-MeV/u Ca-48 beam, are presented. The half-life for 45Cl beta decay is measured to be 513(36) ms. The beta(-) and beta(-)1n decay of Cl-45 populated excited states in Ar-45,Ar-44, respectively. On the basis of gamma-ray singles and gamma-gamma coincidence data, decay schemes for the two daughter nuclei have been established. They are compared with shell model calculations using the FSU interaction. The low-lying negative parity states for Ar-45 are well described by a single particle (neutron) occupying orbitals near the Fermi surface, whereas neutron excitations across the N = 20 shell gap are needed to explain the positive-parity states which are expected to be populated in allowed Gamow-Teller beta decay of Cl-45. The highest beta feeding to the 5/2(+) state in Ar-45 from the ground state of Cl-45 points towards a 3/2(+) spin-parity assignment of the ground state of the parent over the other possibility of 1/2(+). The high Q(ss-) value of Cl-45 decay allows for the population of 1p1h states above the neutron separation energy in Ar-45 leading to positive parity states of Ar-44 being populated by removal of one neutron from the sd shell. The spin-parities of the excited levels in Ar-44 are tentatively assigned for the first time by comparison with the shell model calculations. The 2978 keV level of Ar-44 is identified as the excited 0(+) level which could correspond to a different configuration from the ground state.
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