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arXiv 1104.5249astro-ph.HEphysics.plasm-ph
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稀释热相对论束流中的双流状不稳定性和天体物理相对论激波

Two-stream-like instability in dilute hot relativistic beams and astrophysical relativistic shocks

Ehud Nakar, Antoine Bret, Milos Milosavljevic

摘要:

相对论无碰撞激波被认为是有效的粒子加速器。非线性结果的相互作用的加速粒子的前面运行的冲击,所谓的“前体”,与未扰动的等离子体的冲击上游,被认为是促进这些粒子的额外加速,并可能修改的流体动力学结构的冲击。本文研究了在非磁化和弱磁化等离子体中传播的相对论激波中,激波上游相互作用中出现的动力学模的线性增长:静电双流平行模和静电斜模。这些模式是特别感兴趣的,因为它们是这种类型的系统中已知的增长最快的模式。使用一个简化的分布函数的稀释超相对论性光束,相对论热在自己的休息框架,但有动量,窄准直在冷上游等离子体的框架,它传播到,我们确定了最快的增长模式在整个$k$空间,并计算其增长率。我们考虑所有类型的等离子体(对和离子电子)和光束(带电和电荷中性)。我们发现,不稳定的静电模式存在于任何类型的等离子体和任何冲击参数。我们进一步发现,两个模式,一个平行(PDMATHAMN)和另一个倾斜($k_\perp \sim k_\|$),是竞争优势和任何一个可能主导的增长率在不同区域的相空间。主导模式主要由上游坐标系中加速粒子动量的垂直分布决定,它反映了激波的洛伦兹因子。平行模式在具有较低洛伦兹因子的冲击中变得更占主导地位(即,具有较大的动量扩散)。我们简要地讨论了我们的结果可能的影响,在伽马射线暴源的外部冲击。

英文摘要:

Relativistic collisionless shocks are believed to be efficient particle accelerators. Nonlinear outcome of the interaction of accelerated particles that run ahead of the shock, the so-called "precursor", with the unperturbed plasma of the shock upstream, is thought to facilitate additional acceleration of these particles and to possibly modify the hydrodynamic structure of the shock. We explore here the linear growth of kinetic modes appearing in the precursor-upstream interaction in relativistic shocks propagating in non and weakly magnetized plasmas: electrostatic two-stream parallel mode and electrostatic oblique modes. These modes are of particular interest because they are the fastest growing modes known in this type of system. Using a simplified distribution function for a dilute ultra-relativistic beam that is relativistically hot in its own rest frame, yet has momenta that are narrowly collimated in the frame of the cold upstream plasma into which it propagates, we identify the fastest growing mode in the full $k$-space and calculate its growth rate. We consider all types of plasma (pairs and ions-electrons) and beam (charged and charge-neutral). We find that unstable electrostatic modes are present in any type of plasma and for any shock parameters. We further find that two modes, one parallel ($k_\perp=0$) and the other one oblique ($k_\perp \sim k_\|$), are competing for dominance and that either one may dominate the growth rate in different regions of the phase space. The dominant mode is determined mostly by the perpendicular spread of the accelerated particle momenta in the upstream frame, which reflects the shock Lorentz factor. The parallel mode becomes more dominant in shocks with lower Lorentz factors (i.e., with larger momentum spreads). We briefly discuss possible implications of our results for external shocks in gamma-ray burst sources.

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