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Massive neutron star with strangeness in a relativistic mean-field model with a high-density cut-off

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arxiv 1801.01984 v1 pith:QQWBURQG submitted 2018-01-06 nucl-th

Massive neutron star with strangeness in a relativistic mean-field model with a high-density cut-off

classification nucl-th
keywords interactionneutrondensitylambdalogarithmicmassmean-fieldmodel
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The properties of strangeness neutron star are studied within relativistic mean-field (RMF) model via including a logarithmic interaction as a function of scalar meson field. This logarithmic interaction, named as the $\sigma$-cut potential, can largely reduce the attractive contributions of scalar meson field at high density without any influence on nuclear structure around normal saturation density. In this work, the TM1 parameter set is chosen as the RMF interaction, while the strengths of logarithmic interaction are constrained by the properties of finite nuclei so that we can obtain a reasonable effective nucleon-nucleon interaction. The hyperons, $\Lambda,~\Sigma$, and $\Xi$ are also considered in neutron stars within this framework, whose coupling constants with mesons are determined by the latest hyperon-nucleon and $\Lambda$-$\Lambda$ potentials extracted from the experimental data of hypernuclei. The maximum mass of neutron star can be larger than two solar mass with these hyperons. Furthermore, the nucleon mass at high density will be saturated due to this additional $\sigma$-cut potential, which is consistent with the conclusions from the microscopic calculations such as, Brueckner-Hartree-Fock theory and quark mean-field model.

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  1. Compact star and compact star matter properties from a baryonic extended linear sigma model with explicit chiral symmetry breaking

    nucl-th 2025-12 reject novelty 5.0

    Tuning the πN sigma term to about -600 MeV (or incompressibility to ~500 MeV) lets one RMF model match neutron-star observations, but the tuning is fitting, not prediction.