A new method of solving Vlasov's equation for a crystal is examined. The advantage of this method is that it is possible in some cases to obtain a solution of this equation in finite form for any temperature, which does not contain series. In other cases the solution of the equa tion is found in the form of a series for a certain small parameter which does not contain the temperature. This method enables the solutions obtained by Vlasov for two limitiag cases to be connected.
Department of Theoretical Physics
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