Abstract

In this work we use the equation of state (EOS) of (2+1)-flavor Nambu-Jona-Lasinio (NJL) model to study the structure of the strange quark star. With a new free parameter $\alpha$, the Lagrangian is constructed by two parts, the original NJL Lagrangian and the Fierz transformation of it, as $\mathcal{L}=(1-\alpha)\mathcal{L}_{NJL}+\alpha\mathcal{L}_{Fierz}$. To determine the range of $\alpha$, we compare the binding energies in the 2-flavor and (2+1)-flavor cases. We also consider the constraints of chemical equilibrium and electric charge neutrality in the strange quark star and choose six representative EOSs with different $\alpha$ and $B$ (bag constant) to study their influence on the structure of the strange quark star. As a result, we find that a larger $\alpha$ and a smaller $B$ corresponds to a heavier star with a stiffer EOS. Furthermore, the heaviest strange quark star is in agreement with not only the recent mass observation of PSR J0740+6620 and the X-ray observations on radius measurements, but also the constraint on tidal deformability of GW170817.

Highlights

  • The equation of state (EOS) plays a critical role in the study of the neutron star

  • The nonstrange quark star has been studied for the two-flavor case [13,14], and the results satisfy both the two solar mass constraint from PSR J0348 þ 0432 [2] and the tidal deformability constraint Λð1.4 M⊙Þ ≤ 800 from GW170817 in the previous study [6]

  • II, we introduce the EOS of the strange quark star with the modified (2 þ 1)-flavor NJL model

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Summary

INTRODUCTION

The equation of state (EOS) plays a critical role in the study of the neutron star. Substituting an EOS into the Tolman-Oppenheimer-Volkoff (TOV) equation, we can get the corresponding mass-radius relation of the star. In a recent study [44], the authors propose a modified NJL model containing both the original model Lagrangian and the Fierz transformation of it with the parameter (1 − α) and α adjusting the weight of these two parts, respectively, producing stiffer EOSs than before In this scheme, the nonstrange quark star has been studied for the two-flavor case [13,14], and the results satisfy both the two solar mass constraint from PSR J0348 þ 0432 [2] and the tidal deformability constraint Λð1.4 M⊙Þ ≤ 800 from GW170817 in the previous study [6]. The mass-radius relation and the tidal deformability of the strange quark star with the corresponding EOS are studied.

EOS OF THE STRANGE QUARK MATTER WITH THE NJL MODEL
STRUCTURE OF THE STRANGE QUARK STAR
SUMMARY AND DISCUSSION
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