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Nonrelativistic collisionless shocks in weakly magnetized electron--ion plasmas: two-dimensional particle-in-cell simulation of perpendicular shock

机译:弱磁化电子 - 离子中的非相对论无碰撞冲击   等离子体:垂直冲击的二维粒子模拟

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摘要

A two-dimensional particle-in-cell simulation is performed to investigateweakly magnetized perpendicular shocks with a magnetization parameter of 6 x10^-5, which is equivalent to a high Alfv\'en Mach number M_A of ~130. It isshown that current filaments form in the foot region of the shock due to theion-beam--Weibel instability (or the ion filamentation instability) and thatthey generate a strong magnetic field there. In the downstream region, thesecurrent filaments also generate a tangled magnetic field that is typically 15times stronger than the upstream magnetic field. The thermal energies ofelectrons and ions in the downstream region are not in equipartition and theirtemperature ratio is T_e / T_i ~ 0.3 - 0.4. Efficient electron acceleration wasnot observed in our simulation, although a fraction of the ions are acceleratedslightly on reflection at the shock. The simulation results agree very wellwith the Rankine-Hugoniot relations. It is also shown that electrons and ionsare heated in the foot region by the Buneman instability (for electrons) andthe ion-acoustic instability (for both electrons and ions). However, the growthrate of the Buneman instability is significantly reduced due to the relativelyhigh temperature of the reflected ions. For the same reason, ion-ion streaminginstability does not grow in the foot region.
机译:进行了二维单元格内粒子模拟,以研究磁化参数为6 x10 ^ -5的弱磁化垂直震动,这相当于〜130的高Alfv'en马赫数M_A。结果表明,由于离子束-魏贝尔不稳定性(或离子丝化不稳定性)而在冲击的脚部形成了电流丝,并在此处产生强磁场。在下游区域,这些电流丝还产生纠缠的磁场,该磁场通常比上游磁场强15倍。下游区域的电子和离子的热能不均等,它们的温度比为T_e / T_i〜0.3-0.4。在我们的模拟中未观察到有效的电子加速,尽管一小部分离子在震动反射时略微加速。仿真结果与兰金-Hugoniot关系非常吻合。还表明,由于布尼曼不稳定性(对于电子)和离子声不稳定性(对于电子和离子),在脚部区域中电子和离子被加热。但是,由于反射离子的温度相对较高,Buneman不稳定性的增长率大大降低。出于相同的原因,离子-离子流的不稳定性在足部区域不会增加。

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