AbstractAbstract
[en] Shell-model calculations are performed for the odd- and even-parity states of 39Cl and the odd-parity states of 39S. The 39S odd-parity states and the 39Cl even-parity states were considered in full (1s,0d)20(0f,1p)3 and (1s,0d)21(0f,1p)2 configurational spaces, respectively. For the 39Cl odd-parity states it was necessary to use a highly truncated (1s,0d)20(0f,1p)3 configurational space. The method and results of truncation are discussed in some detail. Observables calculated include energy spectra, binding energies, 40Ar→39Cl+p spectroscopic factors, first-forbidden and allowed β- decay of 39S, and γ transitions in both 39S and 39Cl. Results are compared to experiment. For example, the spectroscopic factors for 1/2+ and 3/2+39Cl states and the γ transitions between the even-parity 39Cl states are predicted with high accuracy while the half-life of 39S is calculated to be 5.6 s (if the spin-parity of 39S has the preferred value of 7/2-) as compared to the experimental value of 11.5±0.5 s
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ANGULAR MOMENTUM, BETA DECAY, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, CHLORINE ISOTOPES, DECAY, ENERGY, EVEN-ODD NUCLEI, ISOTOPES, LIGHT NUCLEI, MATHEMATICAL MODELS, MINUTES LIVING RADIOISOTOPES, NUCLEAR DECAY, NUCLEAR MODELS, NUCLEI, ODD-EVEN NUCLEI, PARTICLE PROPERTIES, RADIOISOTOPES, SECONDS LIVING RADIOISOTOPES, SPECTRA, SULFUR ISOTOPES
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