Abstract
Knowledge of the equation of state (EoS) of cold and dense baryonic matter is essential for the description of properties of neutron stars (NSs). With an increase of the density, new baryon species can appear in NS matter, as well as various meson condensates. In previous works, we developed relativistic mean-field (RMF) models with hyperons and Δ -isobars, which passed the majority of known experimental constraints, including the existence of a 2 M ⊙ neutron star. In this contribution, we present results of the inclusion of ρ − -meson condensation into these models. We have shown that, in one class of the models (so-called KVOR-based models, in which the additional stiffening procedure is introduced in the isoscalar sector), the condensation gives only a small contribution to the EoS. In another class of the models (MKVOR-based models with additional stiffening in isovector sector), the condensation can lead to a first-order phase transition and a substantial decrease of the NS mass. Nevertheless, in all resulting models, the condensation does not spoil the description of the experimental constraints.
Highlights
The equation of state (EoS) of strongly interacting hadronic matter is an essential input for describing the properties of neutron stars (NSs)
We present the results of the inclusion of the ρ− condensate into the MKVOR* model with the universal mass scaling and check the sensitivity of the results to varying the scaling functions
We studied a possibility of charged ρ-meson condensation in a realistic relativistic mean-field model MKVOR* with scaled hadron masses and couplings
Summary
The equation of state (EoS) of strongly interacting hadronic matter is an essential input for describing the properties of neutron stars (NSs). EoS is to pass simultaneously the maximum NS mass constraint, requiring the EoS to be stiff, and the so-called flow constraint [3] coming from the analysis of flows in heavy ion collisions, which requires a soft EoS. This is hard to achieve within traditional models. In most of known model, this leads to a decrease of the maximum NS mass to unrealistic values Another reason of the EoS softening is the possible appearance of the charged ρ-meson condensate in NS matter [5]. More details on the calculations can be found in [7]
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