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    Properties and microscopic structures of dense stellar matter in relativistic mean field models

    Jia-Xing Niu1, Hao Sun1, Cheng-Jun Xia1,*, and Toshiki Maruyama2

    • 1Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University, Yangzhou 225009, China
    • 2Advanced Science Research Center, Japan Atomic Energy Agency, Shirakata 2-4, Tokai, Ibaraki 319-1195, Japan

    • *Contact author: cjxia@yzu.edu.cn

    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 Yp=0.01–0.65 and baryon number densities nb=10−8–2fm−3 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 nb=7.6×10−11–2fm−3 are obtained as well fulfilling β-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 nb≲0.19fm−3 and at larger densities only TW99 gives satisfactory predictions. In general, the dense stellar matter exhibits droplet phase at nb≲0.015fm−3, while more exotic structures such as rods, slabs, tubes, and bubbles appear sequentially as density increases. The critical proton fractions Ypdrip (≈0.26–0.31) for neutron drip are obtained, where neutron gas emerges outside of nuclei at Yp<Ypdrip. For dense stellar matter at small densities (nb≲10−5fm−3) or large proton fractions (nb≲0.1fm−3 and Yp≳Ypdrip), the EOSs and microscopic structures are generally insensitive to the adopted density functionals. With the onset of neutron drip at Yp≲Ypdrip, the uncertainties emerge and peak at nb≈0.02fm−3 within the range 10−5≲nb≲0.1fm−3. At nb≳0.1fm−3, the dense stellar matter becomes uniform and muons eventually appear, where the uncertainties in the EOSs grow significantly.

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