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Relativistic collisionless shocks formation in pair plasmas

机译:对等离子体中相对论无碰撞冲击的形成

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Collisionless shocks are ubiquitous in astrophysics and in the laboratory. Recent numerical simulations and experiments have shown how these can arise from the encounter of two collisionless plasma shells. When the shells interpenetrate, the overlapping region turns unstable, triggering the shock formation. As a first step toward a microscopic understanding of the process, we here analyze in detail the initial instability phase. On the one hand, 2D relativistic PIC simulations are performed where two unmagnetized, symmetric, and initially cold pair plasmas collide. On the other hand, the instabilities at work are analyzed, as well as the field at saturation and the seed field which gets amplified. For mildly relativistic motions and onward, Weibel modes with ω=0+iδ govern the linear phase. We derive an expression for the duration of the linear phase in reasonable agreement with the simulations.
机译:无碰撞冲击在天体物理学和实验室中无处不在。最近的数值模拟和实验表明,如何通过遇到两个无碰撞的等离子壳而产生这些现象。当壳穿透时,重叠区域变得不稳定,从而引发冲击。作为对过程进行微观了解的第一步,我们在这里详细分析初始的​​不稳定性阶段。一方面,在两个未磁化,对称且最初为冷对等离子体碰撞的地方执行了二维相对论PIC仿真。另一方面,分析了工作中的不稳定性以及饱和场和被放大的种子场。对于轻度相对论运动及以后,ω= 0 +iδ的Weibel模式控制线性相位。我们得出与仿真合理一致的线性相位持续时间的表达式。

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