Abstract

We obtain the general expression of the gluon propagator at finite temperature ($T$) and in a magnetic field ($B$), for the case that the four transverse tensor structures appear in the gluon self-energy. By using this expression and a specific form of the one-loop gluon self-energy in the lowest Landau level approximation, we analyze the gluon spectrum in the strong magnetic field limit. As a result, we find that there exist two collective excitations of which the energies are of the order of $p\ensuremath{\sim}gT$ with $g$ being the coupling constant. One of the two excitations enjoys properties quite different from those of the collective excitations at $B=0$ which have been discussed by using the hard thermal loop approximation. We also discuss the static and dynamical screening effects, which are expected to be important for computation of transport coefficients in strong magnetic fields.

Highlights

  • The extreme state of matter created by the relativistic heavy-ion collisions provides us with an opportunity to investigate the dynamics governed by quantum chromodynamics (QCD) at high temperature (T)

  • We obtain the general expression of the gluon propagator at finite temperature (T) and in a magnetic field (B), for the case that the four transverse tensor structures appear in the gluon self-energy

  • We investigate the general expression of the gluon propagator at finite temperature and in a magnetic field, assuming the four transverse tensor components in the gluon self-energy that have been known to appear in the perturbative calculation [35,36,37,38,39,40,41]

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Summary

INTRODUCTION

The extreme state of matter created by the relativistic heavy-ion collisions provides us with an opportunity to investigate the dynamics governed by quantum chromodynamics (QCD) at high temperature (T). A number of theoretical studies have addressed the properties of the extreme QCD matter called the quark-gluon plasma (QGP) Recent studies, both in theory and experiment, suggest opportunities of studying novel properties of the QGP in the strong magnetic field (B) which is thought to be induced in the heavy-ion collisions [1,2,3,4,5] Both in theory and experiment, suggest opportunities of studying novel properties of the QGP in the strong magnetic field (B) which is thought to be induced in the heavy-ion collisions [1,2,3,4,5] We evaluate the gluon propagator in the Coulomb gauge in Appendix A, and summarize the properties of the projection tensors used in order to evaluate the gluon propagator in Appendix B

GENERAL FORM OF GLUON PROPAGATOR
General momentum
Special momenta
ONE-LOOP APPROXIMATION
Collective excitations
Debye screening
Dynamical screening
Brief summary of whole momentum ranges
SUMMARY
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