A parametrized quasiparticle model fitted to finite-magnetic-field lattice QCD thermodynamics predicts that magnetic fields and QCD interactions suppress the shear viscosity and electrical conductivity of the quark-gluon plasma.
Viscous coefficients and thermal conductivity of a $\pi K N$ gas mixture in the medium
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abstract
The temperature and density dependence of the relaxation times, thermal conductivity, shear viscosity and bulk viscosity for a hot and dense gas consisting of pions, kaons and nucleons have been evaluated in the kinetic theory approach. The in-medium cross-sections for $\pi\pi$, $\pi K$ and $\pi N$ scatterings were obtained by using complete propagators for the exchanged $\rho$, $\sigma$, $K^*$ and $\Delta$ excitations derived using thermal field theoretic techniques. Notable deviations can be observed in the temperature dependence of $\eta$, $\zeta$ and $\lambda$ when compared with corresponding calculations using vacuum cross-sections usually employed in the literature. The value of the specific shear viscosity $\eta/s$ is found to be in agreement with available estimates.
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From Non-interacting to Interacting Picture of Quark Gluon Plasma in presence of magnetic field and its fluid property
A parametrized quasiparticle model fitted to finite-magnetic-field lattice QCD thermodynamics predicts that magnetic fields and QCD interactions suppress the shear viscosity and electrical conductivity of the quark-gluon plasma.