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Particle-In-Cell simulations of circularly polarised Alfven wave phase mixing: a new mechanism for electron acceleration in collisionless plasmas

机译:圆极化Alfven波相混合的粒子模拟:无碰撞等离子体中电子加速的新机制

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摘要

Particle-In-Cell simulations of a circularly polarised Alfven wave interaction with one dimensional, across the uniform magnetic field, plasma density inhomogeneity (phase mixing) in collisionless plasmas were performed. In our preliminary work (Tsiklauri et al. 2004, astro-ph/0409537) we reported discovery of a new electron acceleration mechanism. In this mechanism, progressive distortion of Alfven wave front, due to the differences in local Alfven speed, generates oblique (nearly parallel to the magnetic field) electrostatic fields, which accelerate electrons through the Landau resonance. Here we report detailed study of this novel effect, including analysis of broadening of ion distribution function due to the presence of Alfven waves and the generation of compressive perturbations due to weak non-linearity and plasma density inhomogeneity. The amplitude decay law in the inhomogeneous regions, in the kinetic regime, is shown to be the same as in the MHD approximation described by Heyvaerts and Priest (1983).
机译:进行了圆极化Alfven波在均匀磁场,无碰撞等离子体中的等离子体密度不均匀性(相混合)的一维粒子间相互作用模拟。在我们的初步工作中(Tsiklauri等,2004,astro-ph / 0409537),我们报告了新的电子加速机制的发现。在这种机制下,由于局部Alfven速度的差异,Alfven波前的渐进畸变会产生倾斜的(几乎平行于磁场)静电场,从而加速电子通过Landau共振。在这里,我们报告了对这种新型效应的详细研究,包括分析由于Alfven波的存在而引起的离子分布函数的展宽以及由于弱的非线性和等离子体密度的不均匀性而产生的压缩扰动。在动力学范围内,非均匀区域中的振幅衰减定律与Heyvaerts和Priest(1983)所描述的MHD近似相同。

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