Magnetohydrodynamics of strongly magnetized relativistic fluids is derived in
the ideal and dissipative cases, taking into account the breaking of spatial
symmetries by a quantizing magnetic field. A complete set of transport
coefficients, consistent with the Curie and Onsager principles, is derived for
thermal conduction, as well as shear and bulk viscosities. It is shown that in
the most general case the dissipative function contains five shear viscosities,
two bulk viscosities, and three thermal conductivity coefficients. We use
Zubarev's non-equilibrium statistical operator method to relate these transport
coefficients to correlation functions of equilibrium theory. The desired
relations emerge at linear order in the expansion of the non-equilibrium
statistical operator with respect to the gradients of relevant statistical
parameters (temperature, chemical potential, and velocity.) The transport
coefficients are cast in a form that can be conveniently computed using
equilibrium (imaginary-time) infrared Green's functions defined with respect to
the equilibrium statistical operator.Comment: v2: typos corrected, 32 pages, no figures, matches published versio