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PIC Simulation of a quasi-parallel collisionless shock: Interaction between upstream waves and backstreaming ions

机译:PIC仿真对准直接碰撞的冲击:上游波与后射离的相互作用

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摘要

We perform a one-dimensional full particle-in-cell (PIC) simulation of a quasi-parallel collisionless shock with the Alfven Mach number 6.6 and a shock angle of 20 degrees between the upstream magnetic field and the shock normal direction. The backstreaming ions are self-consistently generated by reflections of the incoming ions at the shock. They generate the Alfvenic electromagnetic wave via the right-handed resonant ion-ion instability, as the ions travel toward the upstream region. The energy distribution of the backstreaming ions far upstream splits into two populations as it approaches the shock. The energy threshold of the populations is approximately the energy gained by a single specular reflection at the shock. The maximum energy of the backstreaming ions near the shock is about 10 times larger than the specularly reflected ion energy. Nonlinear phase bunches of the highenergy backstreaming ions and the background ions are found near the shock, due to the resonant and non-resonant trappings by the excited waves, respectively.
机译:我们执行与Alfven Mach编号6.6的准平行碰撞冲击的一维的全粒子 - 电池(PIC)模拟,在上游磁场和冲击正常方向之间的20度的冲击角。后射离离子是通过休克进入离子的反射来自始于自始终产生的。当离子朝向上游区域行进时,它们通过右下谐振离子离子不稳定性产生抗粘性电磁波。在震动接近震动时,后游离子的能量分布将分为两个群体。群体的能量阈值大致通过休克在休克时通过单镜面反射获得的能量。休克附近的后游离子的最大能量比镜面反射离子能量大约10倍。由于激发波的共振和非共振捕获,在冲击附近,在休克附近发现了高中的非线性相位束和背景离子。

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