Abstract

Using complex Langevin dynamics we examine the phase structure of complex unitary matrix models and compare the numerical results with analytic results found at large $N$. The actions we consider are manifestly complex, and thus the dominant contribution to the path integral comes from the space of complexified gauge field configuration. For this reason, the eigenvalues of unitary matrix lie off the unit circle and venture out in the complex plane. One example of a complex unitary matrix model, with Polyakov line as the unitary matrix, is an effective description of a QCD at finite density and temperature with $N$ number of colors and $N_f$ number of quark flavors defined on the manifold $S^1 \times S^3$. A distinct feature of this model, the occurrence of a series of Gross-Witten-Wadia transitions, as a function of the quark chemical potential, is reproduced using complex Langevin simulations. We simulate several other observables including Polyakov lines and quark number density, for large $N$ and $N_f$ and found excellent match with the analytic results.

Highlights

  • A nonperturbative study of the phase structure of QCD at finite temperature and nonzero baryon chemical potential still remains an outstanding problem [1,2]

  • One method is the use of complex Langevin dynamics with stochastic quantization [3,4]

  • We started with a simple matrix model called the ab-model and investigated its phase structure analytically and numerically

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Summary

INTRODUCTION

A nonperturbative study of the phase structure of QCD at finite temperature and nonzero baryon chemical potential still remains an outstanding problem [1,2]. When the chemical potential passes one of the quark energy levels there is a third order Gross-Witten-Wadia (GWW) transition from a confined to a deconfined phase and back again. This model exhibits another interesting feature known as the Silver Blaze behavior. IV we discuss another interesting large N unitary matrix model, which arises in the one-loop formulation of QCD on compact spaces This model possess a tower of quark energy levels due to compactification and is defined for positive and negative chemical potential values. We think that these diagnostics need further investigations and we save it for future work

COMPLEX LANGEVIN DYNAMICS
N θiðτÞ: ð4Þ
Oij j ηj ðτÞ ð7Þ
AB-MODEL
Ungapped phase
Gapped phase
Phase transition of ab-model
GAUGE THEORY TO UNITARY MATRIX MODEL
Observables
Single level model with positive chemical potential
Single level model with interaction
CONCLUSIONS AND DISCUSSIONS
Pressure hpi and energy hEi
Full Text
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