Abstract

We discuss the extension of gauge-invariant electric and magnetic screening masses in the Quark-Gluon Plasma to the case of a finite baryon density, defining them in terms of a matrix of Polyakov loop correlators. We present lattice results for $N_f=2+1$ QCD with physical quark masses, obtained using the imaginary chemical potential approach, which indicate that the screening masses increase as a function of $\mu_B$. A separate analysis is carried out for the theoretically interesting case $\mu_B/T=3 i \pi$, where charge conjugation is not explicitly broken and the usual definition of the screening masses can be used for temperatures below the Roberge-Weiss transition. Finally, we investigate the dependence of the static quark free energy on the baryon chemical potential, showing that it is a decreasing function of $\mu_B$ which displays a peculiar behavior as the pseudocritical transition temperature at $\mu_B=0$ is approached.

Highlights

  • Static color charges are useful probes of the properties of strongly interacting matter

  • We present lattice results for Nf 1⁄4 2 þ 1 QCD with physical quark masses, obtained using the imaginary chemical potential approach, which indicate that the screening masses increase as a function of μB

  • We investigate the dependence of the static quark free energy on the baryon chemical potential, showing that it is a decreasing function of μB, which displays a peculiar behavior as the pseudocritical transition temperature at μB 1⁄4 0 is approached

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Summary

INTRODUCTION

Static color charges are useful probes of the properties of strongly interacting matter. One expects an increase of screening effects as a function of μB, since a finite baryon density favors the onset of deconfinement; this is confirmed by perturbative predictions [14] and by lattice QCD studies considering correlators projected over color representations after gauge fixing [15] In this case, when considering gauge-invariant screening masses, one has to face the problem that charge conjugation symmetry is explicitly broken by the presence of the baryon chemical potential, so a clear separation into electric and magnetic sectors cannot be performed anymore [4].

OBSERVABLES AND NUMERICAL METHODS
The special case of the Roberge-Weiss point
Dependence of the free energy on μB
Simulation details
Screening masses
Results on the dependence of the quark free energy on μB
Magnetic and electric screening masses close to the Roberge-Weiss endpoint
CONCLUSIONS
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