Abstract

The expressions of the shear viscosity and the bulk viscosity components in the presence of an arbitrary external magnetic field for a system of hot charged scalar bosons (spin 0) as well as for a system of hot charged Dirac fermions (spin $\frac{1}{2}$) have been derived by employing the one-loop Kubo formalism. This is done by explicitly evaluating the thermomagnetic spectral functions of the energy-momentum tensors using the real time formalism of finite temperature field theory and the Schwinger proper time formalism. In the present work, a rich quantum field theoretical structure in the expressions of the viscous coefficients in nonzero magnetic field are found, which are different from their respective expressions obtained earlier via kinetic-theory-based calculations; though, in the absence of a magnetic field, the one-loop Kubo and the kinetic-theory-based expressions for the viscosities are known to be identical. We have identified that Kubo and kinetic-theory-based results of viscosity components follow a similar kind of temperature and magnetic field dependency. The relaxation time and the synchrotron frequency in the kinetic theory formalism are realized to be connected, respectively, with the thermal width of propagator and the transitions among the Landau levels of the charged particles in the Kubo formalism. We believe that the connection of the latter quantities is quite new and probably the present work is the first time addressing this interpretation along with the new expressions of viscosity components, not seen in existing works.

Highlights

  • The heavy ion collision experiment at relativistic energy can produce a superhot quark gluon plasma, which may be exposed under a strong magnetic field B if the nucleusnucleus collision is noncentral

  • We will try to explore the numerical outcomes of shear and bulk viscosity components; mainly, their temperature and magnetic-field-dependent curves will be our matter of interest

  • We have performed a detailed calculation of the one-loop Kubo expressions of the five shear viscosity components and the two bulk viscosity components in the presence of an arbitrary background magnetic field B, where a general form of the thermomagnetic propagators are used based on the real time formalism of finite temperature field theory and the Schwinger proper time formalism

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Summary

INTRODUCTION

The heavy ion collision experiment at relativistic energy can produce a superhot quark gluon plasma, which may be exposed under a strong magnetic field B if the nucleusnucleus collision is noncentral. A quantum field theoretical treatment at finite temperature and magnetic field via the Kubo relations has never been attempted in details which could reveal rich quantum structure in shear and bulk viscosity components. As far as our best knowledge, we are going to address for the first time a one-loop Kubo expression of viscosity components in the presence of a magnetic field by using a real time formalism of finite temperature field theory and the Schwinger proper time framework. To compensate the calculation gaps, we have provided detailed Appendixes at the end

THE SPECTRAL FUNCTION OF THE ENERGY-MOMENTUM TENSOR
VISCOUS COEFFICIENTS FROM THE SPECTRAL FUNCTION IN KUBO FORMALISM
NUMERICAL RESULTS AND DISCUSSIONS
SUMMARY AND CONCLUSION
C T μDνirac ðxÞT αDβirac ðyÞi11
C T μscνalar ðxÞT αscβalar ðyÞiB11
T2 g ω2kfaðωkÞf1 þ afaðωk
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