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The bipolar non-isentropic compressible Euler-Maxwell system is investigatedin $R^3$ in the present paper, and the $L^q$ time decay rate for the globalsmooth solution is established. It is shown that the total densities, totaltemperatures and magnetic field of two carriers converge to the equilibriumstates at the same rate $(1+t)^{-3/2+3q/2}$ in $L^q$ norm. But, both thedifference of densities and the difference of temperatures of two carriersdecay at the rate $(1+t)^{-2-\frac{1}{q}}$, and the velocity and electric fielddecay at the rate $(1+t)^{-3/2+\frac{1}{2q}}$. This phenomenon on the chargetransport shows the essential difference between the non-isentropic unipolarEuler-Maxwell and the bipolar isentropic Euler-Maxwell system.

The asymptotic behavior of globally smooth solutions of bipolar non-isentropic compressible Euler-Maxwell system for plasma