The electrical conductivity of a fully ionized magnetic plasma with screened interaction between charges

The method of solving the kinetic Boltzmann equation is used to calculate the electrical conductivity of a fully ionized plasma with screened interaction between charges, located in a time-constant external magnetic field. The dependence of the longitudinal, transverse, and Hall conductivity on the nonideality parameter $\Gamma$ of the plasma and on the parameter $\omega_e\tau_0$ is established. It is demonstrated that the maximum (modulo) value of the Hall components of plasma conductivity shifts towards lower values of the intensity $H$ of external magnetic field as the nonideality parameter $\Gamma$ increases.