重新审视拟线性理论的有效性

Y.‐M. Liang, P. Diamond
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引用次数: 19

摘要

讨论了一维单种等离子体中Langmuir波的弱湍流理论。利用两点关联理论进行的分析计算表明,在弱湍流状态下,τac≪min(τtr,γ - 1k)(其中τac是场自相关时间,τtr是粒子去相关时间),模态生长速率γk在弱湍流膨胀参数中超出线性、朗道生长速率γ kl的非线性增强很小,是可加性的,且阶数较高。因此,这一结果支持了Langmuir波湍流的拟线性理论的有效性,并与Adam、Laval和Pesme[物理学家]的预测不一致。[j] . Rev. Lett. 43, 1671(1979)],这表明在τac≪τtr≪γ - 1k方面有不可忽视的乘法增强。分析表明,他们的结果是由于使用了一个无效的波动源项。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Revisiting the validity of quasilinear theory
The weak turbulence theory of Langmuir waves in a one‐dimensional, one‐species plasma is discussed. Analytic calculations using the theory of two‐point correlations show that in the weak turbulence regime, τac≪min(τtr,γ−1k) (where τac is the field autocorrelation time and τtr is the particle decorrelation time), the nonlinear enhancement of the mode growth rate γk beyond the linear, Landau growth rate γkL is small, additive, and higher order in the weak turbulence expansion parameter. This result thus supports the validity of the quasilinear theory for Langmuir wave turbulence, and disagrees with the predictions of Adam, Laval, and Pesme [Phys. Rev. Lett. 43, 1671 (1979)], which indicate a non‐negligible, multiplicative enhancement in the regime τac≪τtr≪γ−1k. Analysis shows that their result comes from the use of an invalid source term for the fluctuations.
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