Properties and microscopic structures of dense stellar matter in relativistic mean field models
Phys. Rev. C 113, 025804 – Published 11 February, 2026
DOI: https://doi.org/10.1103/x9fk-ykm1
Abstract
Data tables on the equation of state (EOS) and microscopic structures for cold dense stellar matter with proton fractions –0.65 and baryon number densities are obtained adopting 13 different relativistic density functionals, i.e., NL3, PK1, PK1r, GM1, MTVTC, DD-LZ1, PKDD, DD-ME2, TW99, DD-MEX, DD-MEX1, DD-MEX2, and DD-MEY. The EOSs of dense stellar matter inside neutron stars with baryon number densities are obtained as well fulfilling -stability condition, where those with TW99, DD-MEY, DD-MEX1, DD-ME2, DD-MEX, and DD-LZ1 are generally consistent with the constraints obtained by Huth et al. [Nature (London) 606, 276 (2022)] at and at larger densities only TW99 gives satisfactory predictions. In general, the dense stellar matter exhibits droplet phase at , while more exotic structures such as rods, slabs, tubes, and bubbles appear sequentially as density increases. The critical proton fractions (–0.31) for neutron drip are obtained, where neutron gas emerges outside of nuclei at . For dense stellar matter at small densities () or large proton fractions ( and ), the EOSs and microscopic structures are generally insensitive to the adopted density functionals. With the onset of neutron drip at , the uncertainties emerge and peak at within the range . At , the dense stellar matter becomes uniform and muons eventually appear, where the uncertainties in the EOSs grow significantly.