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Weakly nonlinear waves in magnetized plasma with a slightly non-Maxwellian electron distribution. Part 1. Stability of solitary waves

机译:磁化等离子体中的弱非线性波,具有稍微非麦克斯韦电子分布。第1部分。孤波的稳定性

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Weakly nonlinear waves in strongly magnetized plasma with slightly non-isothermal electrons are governed by a modified Zakharov-Kuznetsov (ZK) equation, containing both quadratic and half-order nonlinear terms, which we refer to as the Schamel-Korteweg-de Vries-Zakharov-Kuznetsov (SKdVZK) equation. We present a, method to obtain an approximation for the growth rate, gamma, of sinusoidal perpendicular perturbations of wavenumber, k. to SKdVZK solitary waves over the entire range of instability. Unlike for (modified) ZK equations with one nonlinear term, in this method there is no analytical expression for k(c), the cut-off wavenumber (at which the growth rate is zero) or its corresponding eigenfunction. We therefore obtain approximate expressions for these using an expansion parameter, a, related to the ratio of the nonlinear terms. The expressions are then Used to find gamma for k near k(c) as a function of a The approximant derived from combining these analytical results with the ones for small k agrees very well with the values of gamma obtained numerically. It is found that both k(c) and the maximum growth rate decrease as the electron distribution becomes progressively less peaked than the Maxwellian. We also present new algebraic and rarefactive solitary wave solutions to the equation.
机译:具有稍微非等温电子的强磁化等离子体中的弱非线性波由修正的Zakharov-Kuznetsov(ZK)方程控制,该方程包含二次和半阶非线性项,我们将其称为Schamel-Korteweg-de Vries-Zakharov -库兹涅佐夫(SKdVZK)方程。我们提出一种方法,以获取波数k的正弦垂直扰动的增长率γ的近似值。在整个不稳定性范围内都受到SKdVZK孤立波的影响。与具有一个非线性项的(修改的)ZK方程不同,在此方法中,没有k(c),截止波数(增长率为零)或其相应本征函数的解析表达式。因此,我们使用与非线性项的比率有关的扩展参数a来获得这些表达式的近似表达式。然后将这些表达式用于根据k的函数找到k附近的k的伽马。将这些分析结果与小k的分析结果相结合得出的近似值与通过数值获得的γ值非常吻合。已经发现,随着电子分布的峰值逐渐变得比麦克斯韦ianian减小,k(c)和最大增长率都降低。我们还为该方程式提供了新的代数和稀疏孤波解。

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