Abstract

I make two comments about nuclear matter. First, I consider the effects of a coupling between the $O(4)$ chiral field, $\vec{\phi}$, and the $\omega_\mu$ meson, $\sim + \, \omega_\mu^2 \, \vec{\phi}^{\, 2}$; for any net baryon density, a condensate for $\omega_0$ is unavoidably generated. I assume that with increasing density, a decrease of the chiral condensate and the effective $\omega_0$ mass gives a stiff equation of state (EoS). In order to match that onto a soft EoS for quarkyonic matter, I consider an $O(N)$ field at large $N$, where at nonzero temperature quantum fluctuations disorder any putative pion "condensate" into a quantum pion liquid (Q$\pi$L) (arXiv:2005.10259). In this paper I show that the Q$\pi$L persists at zero temperature. If valid qualitatively at $N=4$, the $\omega_0$ mass goes up sharply and suppresses the $\omega_0$ condensate. This could generate a spike in the speed of sound at high density, which is of relevance to neutron stars. Second, I propose a toy model of a $Z(3)$ gauge theory with three flavors of fermions, where $Z(3)$ vortices confine fermions into baryons. In $1+1$ dimensions this model can be studied numerically with present techniques, using either classical or quantum computers.

Highlights

  • To determine the equation of state (EOS) for nuclear matter, effective models can be used for baryon densities, nB, up to and above that for nuclear saturation, nsat [1,2,3,4,5,6,7,8,9,10]

  • In the past few years, astronomical observations of neutron stars [11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32] have provided a significant insight into the nuclear EOS at densities above nsat

  • Uð1ÞA symmetry survive at densities far above nsat, as indicated by an analysis using a dilute gas of instantons

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Summary

INTRODUCTION

To determine the equation of state (EOS) for nuclear matter, effective models can be used for baryon densities, nB, up to and above that for nuclear saturation, nsat [1,2,3,4,5,6,7,8,9,10]. In the past few years, astronomical observations of neutron stars [11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32] have provided a significant insight into the nuclear EOS at densities above nsat. Excitations near the Fermi surface are dominated by color superconductivity [33,34,36]

Published by the American Physical Society
The ωμ Lagrangian is
This assumes that processes which violate the axial
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