PaperPanorama

Nuclear Theory·nucl-th

Thursday·March 23, 2023

14 papers2 primary·12 cross-listed

  1. 01

    Neutron Skin Thickness Dependence of Astrophysical -factor

    T. Ghosh · Sangeeta · G. Saxena · B. K. Agrawal · Ushasi Datta

    Background: The density dependence of nuclear symmetry energy is crucial in determining several properties of finite nuclei to the neutron stars with mass 1.4 . The values of neutron skin thickness, isovector giant dipole resonances energies and various nuclear reaction cross-sections in asymmetric nuclei have been utilized to determine the slope of symmetry energy () at the saturation density. Recent PREX-II and CREX measurements of neutron skin thickness in Pb and Ca nuclei yield very different values of which overlap marginally within 90 confidence interval. Purpose: Our objective is to demonstrate the role of symmetry energy on the sub-barrier fusion cross-section and the astrophysical -factor for asymmetric nuclei. Method: The nucleus nucleus potentials are generated using the double folding model (DFM) for three different nucleon-nucleon interactions. These DFM potentials are used for the calculation of the sub-barrier fusion cross-section and the astrophysical -factor. The nucleon densities required for DFM potentials are generated from different families of non-relativistic and relativistic mean-field models which correspond to a wide range of neutron skin thickness or . Results: We have calculated the sub-barrier fusion cross-section for several asymmetric nuclei involving O, Ca, Ni, and Sn isotopes. The results are presented for the barrier parameters, cross-section, and astrophysical -factor for Ca+Ca and Sn+Sn as a function of neutron skin thickness. Conclusions: The cross-section for the neutron-rich nuclei show a strong dependence on the behavior of symmetry energy or the neutron skin thickness. The increase in skin thickness lowers the height of the barrier as well as its width which enhances the values of the -factor by more than an order of magnitude.

    nucl-thastro-ph.HEastro-ph.SR2 citations
  2. 02

    Non-thermal distributions of charm and charmonium in relativistic heavy-ion collisions

    Chaoyu Pan🇨🇳 · Shuhan Zheng🇨🇳 · Meimei Yang🇨🇳 · Zhiwei Liu🇨🇳 · Baoyi Chen🇨🇳

    We employ the Boltzmann transport model to study the charmonium regeneration with non-thermal charm quarks in relativistic heavy-ion collisions. As heavy quarks do not reach kinetic thermalization in the quark-gluon plasma (QGP), the final transverse momentum distribution of regenerated charmonium depends on the degree of charm quark kinetic thermalization. When the charm momentum distribution becomes harder, more charm quarks are distributed in the middle and high , where the production of regenerated charmonium also becomes larger. With non-thermal momentum distribution of charm quarks in their coalescence process, the nuclear modification factor of charmonium enhances at middle . Besides, the elliptic flow of charmonium also enhances at middle as more regenerated charmonium are distributed in this region. The theoretical calculations with non-thermal charm distribution explain well the dependence of charmonium and , which indicates that charm quarks do not reach complete kinetic thermalization in the QGP when charmonium are regenerated.

    nucl-thhep-phPRC(2023)·4 citations

Affiliations

first authorsco-authorsvia INSPIRE