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Envelope equation for the linear and nonlinear propagation of an electron plasma wave, including the effects of Landau damping, trapping, plasma inhomogeneity, and the change in the state of wave

机译:线性和非线性传播的包络方程   电子等离子体波,包括Landau阻尼,陷阱,   等离子体不均匀性和波状态的变化

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摘要

This paper addresses the linear and nonlinear three-dimensional propagationof an electron wave in a collisionless plasma that may be inhomogeneous,nonstationary, anisotropic and even weakly magnetized. The wave amplitude,together with any hydrodynamic quantity characterizing the plasma (density,temperature,...) are supposed to vary very little within one wavelength or onewave period. Hence, the geometrical optics limit is assumed, and the wavepropagation is described by a first order differential equation. This equationexplicitly accounts for three-dimensional effects, plasma inhomogeneity, Landaudamping, and the collisionless dissipation and electron acceleration due totrapping. It is derived by mixing results obtained from a direct resolution ofthe Vlasov-Poisson system and from a variational formalism involving a nonlocalLagrangian density. In a one-dimensional situation, abrupt transitions arepredicted in the coefficients of the wave equation. They occur when the stateof the electron plasma wave changes, from a linear wave to a wave with trappedelectrons. In a three dimensional geometry, the transitions are smoother,especially as regards the nonlinear Landau damping rate, for which a verysimple effective and accurate analytic expression is provided.
机译:本文探讨了在无碰撞等离子体中电子波的线性和非线性三维传播,该碰撞可能是不均匀,不稳定,各向异性甚至弱磁化的。假设在一个波长或一个波周期内,波的振幅以及表征等离子体的任何流体力学量(密度,温度等)的变化很小。因此,假定几何光学极限,并且通过一阶微分方程描述波的传播。该方程式明确地说明了三维效应,等离子不均匀性,Landaudamping以及由于陷获而产生的无碰撞耗散和电子加速度。它是通过混合直接从Vlasov-Poisson系统的分辨率和涉及非局部拉格朗日密度的变式形式而获得的结果而得出的。在一维情况下,波动方程的系数会预测突变。当电子等离子体波的状态从线性波变为电子束缚波时,它们就会发生。在三维几何结构中,过渡更加平滑,尤其是对于非线性Landau阻尼率而言,为此提供了非常简单的有效且精确的解析表达式。

著录项

  • 作者

    Bénisti, Didier;

  • 作者单位
  • 年度 2016
  • 总页数
  • 原文格式 PDF
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  • 中图分类
  • 入库时间 2022-08-20 21:10:15

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