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Collisional effect on the Weibel instability with the bi-Maxwellian distribution function

机译:双向麦克斯韦分布函数对威贝尔不稳定性的碰撞效应

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摘要

In this paper, the Coulomb collision effect of electron-ion is investigated based on the equilibrium bi-Maxwellian anisotropic distribution function in dense and unmagnetized plasma. An analytical expression is derived for the real frequency and the growth rate of the Weibel instability for two limiting cases | ξ = ω ′ k | | θ | | | ? 1 and | ξ | ? 1. In the limit | ξ | ? 1, the quantity η that is due to a collisional term will appear in the growth and condition of the rate of the Weibel instability, which leads to a constraining condition of the growth rate. When η increases, the growth rate will increase and the wave instability will be distant from its own damping mode.
机译:本文基于在稠密和未磁化等离子体中的平衡双麦克斯韦各向异性分布函数研究了电子离子的库仑碰撞效应。对于两个极限情况|导出了Weibel不稳定性的真实频率和增长率的解析表达式。 ξ=ω'k | | θ| | | ? 1和| ξ| ? 1.在极限ξ| ?在图1中,由于碰撞项引起的量η将出现在维贝尔不稳定性的增长率和条件中,这导致增长率的约束条件。当η增加时,增长率将增加并且波的不稳定性将远离其自身的阻尼模式。

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