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本文在Gauss随机过程的基础上建立了描写等离子体强湍流的平均传播量的理论,证明了群的性质,分析了它的物理意义及基本应用,指出这一理论和Misguich-Balescu所提出的RQL弱耦合理论相比是对等离子体强湍流更好的描述。In this papar, a theory of the average propagator U for the plasma turbulence is established on the basis of the Gaussian process. The group properties of U is showed, its physical meaning and the fundamental applications are analyzed. It is pointed out that the theory is a better description for the plasma turbulence compared to the weak coupling EQL theory given by Misguich and Balescu.







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