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Longitudinal dielectric function and dispersion relation of electrostatic waves in relativistic plasmas

机译:静电波在相对论等离子体中的纵向介质函数和色散关系

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摘要

The longitudinal dielectric function is derived analytically from the relativistic Vlasov equation for arbitrary values of the relevant parameters z = mc(2)/T, where m is the rest electron mass, c is the speed of light, and T is the electron temperature in energy units. A new analytical approach based on the Legendre polynomial expansion and continued fractions was used. Analytical expression of the electron distribution function was derived. The real part of the dispersion relation and the damping rate of electron plasma waves are calculated both analytically and numerically in the whole range of the parameter z. The results obtained improve significantly the previous results reported in the literature. For practical purposes, explicit expressions of the real part of the dispersion relation and the damping rate in the range z > 30 and strongly relativistic regime are also proposed.
机译:纵向介质函数是从相关参数Z = MC(2)/ T的任意值的相对论Vlasov方程的相对论Vlasov方程来源的,其中M是其余电子质量,C是光速,而T是电子温度 能量单位。 使用基于Legendre多项式扩增和持续级分的新分析方法。 衍生电子分布函数的分析表达。 分散关系的实际部分和电子等离子体波的阻尼率在参数Z的整个范围内分析和数值计算。 得到的结果显着改善了文献中报告的先前结果。 出于实际目的,还提出了分散关系的实际部分的明确表达和Z> 30范围内的阻尼速率和强相相对的状态。

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