Electrical conductivity and shear viscosity of a pion gas in a thermo-magnetic medium
arXiv:2403.05165 · doi:10.1140/epja/s10050-024-01291-w
Abstract
We evaluate the electrical conductivity and shear viscosity of a interacting pion gas in a thermo-magnetic medium using the kinetic theory. The collision term of the relativistic Boltzmann transport equation in presence of background magnetic field is solved using the relaxation time approximation. The medium modified relaxation time is obtained from the corresponding in-medium scattering cross-section calculated using the thermo-magnetic propagator. It is observed that the average relaxation time shows a variation with temperature for a fixed value of magnetic field. The relaxation time shows a mild oscillatory variation with respect to the magnetic field. It is also observed that the medium dependent scattering cross-section causes a considerable amount of influence on the electrical conductivity and shear viscosity compared to its vacuum counterpart.
Version published in EPJA
References in corpus (10)
- Magnetic-Field-Induced insulator-conductor transition in SU(2) quenched lattice gauge theory
- Chiral Hall Effect and Chiral Electric Waves
- Nonlinear electromagnetic response in quark-gluon plasma
- Transport coefficients of two-flavor superconducting quark matter
- Electrical Conductivity of Dense Quark Matter with Fluctuations and Magnetic Field Included
- Effect of spectral modification of on shear viscosity of a pion gas
- Anisotropic pressure of magnetized quark matter with anomalous magnetic moment
- Magnetic catalysis of a finite size pion condensate
- Charged pseudoscalar and vector meson masses under strong magnetic fields in an extended NJL model
- Finite size effect on the thermodynamics of a hot and magnetized hadron resonance gas