Abstract

Using a nonlocal version of the Polyakov-loop-extended Nambu-Jona-Lasinio model, we investigate effects of a nonderivative vector-current interaction (relating to the quark-number density) at both real and imaginary chemical potentials. This repulsive vector interaction between quarks has the following impact on the chiral first-order phase transition: at imaginary chemical potential it sharpens the transition at the Roberge-Weiss (RW) end point and moves this critical point toward lower temperatures; at real chemical potential, the critical end point moves on a trajectory towards larger chemical potentials and lower temperatures with increasing vector coupling strength. The conditions are discussed at which the first-order phase transition disappears and turns into a smooth crossover.

Highlights

  • Exploring the phase diagram of quantum chromo-dynamics (QCD) at finite temperature and real chemical potential is one of the most interesting and important subjects in particle and nuclear physics

  • This repulsive vector interaction between quarks has the following impact on the chiral first-order phase transition: at imaginary chemical potential it sharpens the transition at the Roberge-Weiss (RW) end point and moves this critical point toward lower temperatures; at real chemical potential, the critical end point moves on a trajectory towards larger chemical potentials and lower temperatures with increasing vector coupling strength

  • LQCD suffers from the so-called sign problem which restricts the applicability of LQCD to the region of small real chemical potential R and high temperatures

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Summary

Introduction

Exploring the phase diagram of quantum chromo-dynamics (QCD) at finite temperature and real chemical potential is one of the most interesting and important subjects in particle and nuclear physics. A promising strategy for studying the QCD phase diagram at finite R is the imaginary-chemical-potential matching approach [3]. In the imaginary-chemical-potential matching approach we extract some important restrictions for the model design from the I region. This allows us to extend the model to the real-chemical-potential region more realistically The Polyakov-loop-extended Nambu-Jona-Lasinio (PNJL) model is a promising approach as it preserves the RW periodicity in the same way as QCD. We describe in detail the treatment of the vector-type interaction in the nonlocal framework We show how this approach can be extended to imaginary chemical potentials.

Lagrangian Density and Nonlocality Distribution Functions
Thermodynamical Potential
A43 A48 2T
Parameter Setting
Numerical Results
Summary

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