Gamow-Teller strength distribution in proton-rich nucleus 57Zn and its implications in astrophysics

Abstract

Gamow-Teller (GT) transitions play a preeminent role in the collapse of stellar core in the stages leading to a Type-II supernova. The microscopically calculated GT strength distributions from ground and excited states are used for the calculation of weak decay rates for the core-collapse supernova dynamics and for probing the concomitant nucleosynthesis problem. The B(GT) strength for 57 Zn is calculated in the domain of proton-neutron Quasiparticle Random Phase Approximation (pn-QRPA) theory. No experimental insertions were made (as usually made in other pn-QRPA calculations of B(GT) strength function) to check the performance of the model for proton-rich nuclei. The calculated B(GT) strength distribution is in good agreement with measurements and shows differences with the earlier reported shell model calculation. The pn-QRPA model reproduced the measured low-lying strength for 57 Zn better in comparison to the KB3G interaction used in the large-scale shell model calculation. The stellar weak rates are sensitive to the location and structure of these low-lying states in daughter 57 Cu. The structure of 57 Cu plays a sumptuous role in the nucleosynthesis of proton-rich nuclei. The primary mechanism for producing such nuclei is the rp-process and is believed to be important in the dynamics of the collapsing supermassive stars. Small changes in the binding and excitation energies can lead to significant modifications of the predictions for the synthesis of proton rich isotopes. The β + -decay and electron capture (EC) rates (FFN). The pn-QRPA calculated β + -decay rates are generally in good agreement with the FFN calculation. However at high stellar temperatures the calculated β + -decay rates are almost half of FFN rates. On the other hand, for rp-process conditions, the calculated electron capture (β + -decay) rates are bigger than FFN rates by more than a factor 2 (1.5) and may have interesting astrophysical consequences.