Abstract

We study the chiral phase transition of quark matter under rotation in two-flavor Nambu--Jona-Lasinio (NJL) model. It is found that, in the rotating frame, the angular velocity plays the similar role as the baryon chemical potential and suppresses the chiral condensate, thus the chiral phase transition shows a critical end point not only in the temperature-chemical potential $T-\mu$ plane, but also in the temperature-angular momentum $T-\omega$ plane. One interesting observation is that in the $T-\mu$ plane, the presence of the angular momentum only shifts down the critical temperature $T^E$ of the CEP and does not shift the critical chemical potential $\mu^E$, and in the $T-\omega$ plane, the increase of the chemical potential only shift down the critical temperature $T^E$ and does not change the critical angular momentum $\omega^E$. The phase structure in the $T-\mu$ plane is sensitive to the coupling strength in the vector channel, while the phase structure in $T-\omega$ plane is not. It is also observed that the rotating angular velocity suppresses the kurtosis of the baryon number fluctuations, while it enhances the pressure density, energy density, the specific heat and the sound velocity.

Highlights

  • The phase transitions and phase structure of quantum chromodynamics (QCD) at finite temperature, density, and other extreme conditions are the main topics of relativistic heavy ion collisions

  • Because the properties we have observed that the angular velocity only shifts down the critical temperature of critical end point (CEP) in the T-μ plane, and the chemical potential only shifts down the critical temperature of CEP in the T-ω plane, we can explicitly see that most part on the phase diagram is crossover, and the first order chiral phase transition only exists in two corners on the surface, i.e., in the corner of small ω and large μ and the corner of small μ and large ω, as shown by blue regions on the graph

  • We investigate the effect of the angular velocity on the chiral phase transition of quark matter in the two-flavor NJL model with vector interaction

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Summary

INTRODUCTION

The phase transitions and phase structure of quantum chromodynamics (QCD) at finite temperature, density, and other extreme conditions are the main topics of relativistic heavy ion collisions. We investigate the QCD phase diagram of fast rotating quark matter at finite temperature and density in the two-flavor NJL model with vector interaction. In recent studies, it is pointed out in [18,20,21,22] that the boundary effect is very important in rotating system, since all the research are considering the leading order of angular velocity in Lagrangian expansion, strictly speaking, this is only true when the angular velocity is much smaller than the inverse of the system’s size and can ignore the finite volume boundary effect.

FORMALISM
NUMERICAL RESULTS
Phase diagram in the T-μ and T-ω plane
The effect of vector interaction on the phase structure
The three-dimensional phase diagram in the T-μ-ω plane
The baryon number susceptibilities
Other thermodynamic quantities
CONCLUSION AND OUTLOOK
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