Quark matter in light neutron stars

TL;DR

This paper investigates how higher-order repulsive interactions in the NJL model affect quark matter stability in light neutron stars, showing that 8-quark interactions enable quark cores at low masses and align with recent astrophysical data.

Contribution

It introduces the role of 8-quark vector-isoscalar interactions in the NJL model to explain stable quark cores in light neutron stars, consistent with recent observations.

Findings

8-quark interactions stiffen the quark matter EoS

Quark cores can appear at neutron star masses around 1 solar mass

Maximum neutron star mass and radius are sensitive to 8-quark interaction strength

Abstract

Higher-order repulsive interactions are included in the three-flavor NJL model in order to describe the quark phase of an hybrid star. The effect of 4-quark and 8-quark vector-isoscalar interactions in the stability of hybrid star configurations is analyzed. The presence of a 8-quark vector-isoscalar channel is seen to be crucial in generating large quark branches in the $M(R)$ diagram. This is due to its stiffening effect on the quark matter equation of state which arises from the non-linear density dependence of the speed of sound. This additional interaction channel allows for the appearance of a quark core at moderately low NS masses, $\sim 1M_{\odot}$, and provides the required repulsion to preserve the star stability up to $\sim2.1M_{\odot}$. Furthermore, we show that both the heaviest NS mass generated, $M_{\text{max}}$, and its radii, $R_{\text{max}}$, are quite sensitive to the strength of 8-quark vector-isoscalar channel, leading to a considerable decrease of $R_{\text{max}}$ as the coupling increases. This behavior imprints a considerable deviation from the purely hadronic matter equation of state in the $\Lambda(M)$ diagram, which might be a possible signature of the quark matter existence, even for moderately low NS masses, $\sim 1.4\, M_\odot$. The resulting $M(R)$ and $\Lambda(R)$ relations are in accordance with the latest astrophysical constraints from NICER and Ligo/VIRGO observations, respectively.