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A nonlinear Monte Carlo model of super-diffusive shock acceleration with magnetic field amplification

机译:一类非线性蒙特卡罗超扩散激波加速模型   磁场放大

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摘要

Fast collisionless shocks in cosmic plasmas convert their kinetic energy flowinto the hot downstream thermal plasma with a substantial fraction of energygoing into a broad spectrum of superthermal charged particles and magneticfluctuations. The superthermal particles can penetrate into the shock upstreamregion producing an extended shock precursor. The cold upstream plasma flow isdecelerated by the force provided by the superthermal particle pressuregradient. In high Mach number collisionless shocks, efficient particleacceleration is likely coupled with turbulent magnetic field amplification(MFA) generated by the anisotropic distribution of accelerated particles. Thisanisotropy is determined by the fast particle transport making the problemstrongly nonlinear and multi-scale. Here, we present a nonlinear Monte Carlomodel of collisionless shock structure with super-diffusive propagation ofhigh-energy Fermi accelerated particles coupled to particle acceleration andMFA which affords a consistent description of strong shocks. A distinctivefeature of the Monte Carlo technique is that it includes the full angularanisotropy of the particle distribution at all precursor positions. The modelreveals that the super-diffusive transport of energetic particles (i.e.,Levy-walk propagation) generates a strong quadruple anisotropy in the precursorparticle distribution. The resultant pressure anisotropy of the high-energyparticles produces a non-resonant mirror-type instability which amplifiescompressible wave modes with wavelengths longer than the gyroradii of thehighest energy protons produced by the shock.
机译:宇宙等离子体中的快速无碰撞冲击将其动能流入热的下游热等离子体中,其中很大一部分能量进入了广谱的超热带电粒子和磁涨落。超热颗粒可以渗透到激波上游区域,从而产生扩展的激波前体。上游的冷等离子体流通过过热颗粒压力梯度提供的力而减速。在高马赫数的无碰撞冲击中,有效的粒子加速可能会与由加速粒子的各向异性分布产生的湍流磁场放大(MFA)耦合。这种各向异性是由快速的粒子传输所决定的,该粒子使该问题成为非线性且多尺度的问题。在这里,我们提出了一种无碰撞冲击结构的非线性蒙特卡洛模型,该结构具有高能费米加速粒子的超扩散传播,以及粒子加速和MFA,可提供对强震的一致描述。蒙特卡罗技术的独特之处在于它包括了所有前驱体位置的粒子分布的全部角各向异性。该模型表明,高能粒子的超扩散传输(即Levy-walk传播)会在前体粒子分布中产生很强的四倍各向异性。高能粒子产生的压力各向异性会产生非共振镜面类型的不稳定性,这种不稳定性会放大可压缩波模式,该波模式的波长比激波产生的最高能量质子的陀螺半径更长。

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