Test-particle simulations of Fermi acceleration of electrons at quasiperpendicular shocks

G. Gisler
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Abstract

Summary form only. A type of first-order Fermi electron acceleration associated with quasi-perpendicular shocks has been studied. Ion-scale transverse waves in the magnetic field upstream of the shock do not scatter electrons. However, when these waves are advanced into the shock, the leading edges are compressed first, producing mirror points for a large fraction of the electrons. Thus a population of electrons is trapped in a flux tube between two such mirror points that converge as the field continues to advect into the shock. A similar trap is formed when straight field lines are advected into a concave region of a corrugated shock. In either case, the population is longitudinally accelerated by compression between converging mirrors. A few electrons, having special initial conditions, can be accelerated by this means to energies thousands of times greater than their injection energies. Starting from a Maxwellian distribution of initial energies, the resulting particle energy spectrum is a mildly heated (factors of two to five) Maxwellian plus a power law to very high energies with an index -2.6.<>
准垂直激波下电子费米加速度的测试粒子模拟
只有摘要形式。研究了一类与准垂直激波有关的一阶费米电子加速度。激波上游磁场中的离子级横波不会散射电子。然而,当这些波进入激波时,前缘首先被压缩,为大部分电子产生镜像点。因此,一群电子被困在两个这样的镜像点之间的通量管中,当场继续平流到激波中时,这两个镜像点会聚。当直线场线平流到波纹激波的凹区域时,形成类似的陷阱。在任何一种情况下,人口是纵向加速的压缩之间的会聚镜。一些具有特殊初始条件的电子可以通过这种方法加速到比注入能量大几千倍的能量。从初始能量的麦克斯韦分布出发,得到的粒子能谱是一个温和加热的(因子2到5)麦克斯韦加上一个指数为-2.6的非常高的能量的幂律。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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