Electron Acceleration at Quasi-parallel Non-relativistic Shocks: A 1D Kinetic Survey

Siddhartha Gupta, Damiano Caprioli, Anatoly Spitkovsky
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Abstract

We present a survey of 1D kinetic particle-in-cell simulations of quasi-parallel non-relativistic shocks to identify the environments favorable for electron acceleration. We explore an unprecedented range of shock speeds $v_{\rm sh}\approx 0.067-0.267\,c$, Alfv\'{e}n Mach numbers $\mathcal{M}_{\rm A} = 5-40$, sonic Mach numbers $\mathcal{M}_{\rm s} = 5-160$, as well as the proton-to-electron mass ratios $m_{\rm i}/m_{\rm e}=16-1836$. We find that high Alfv\'{e}n Mach number shocks can channel a large fraction of their kinetic energy into nonthermal particles, self-sustaining magnetic turbulence and acceleration to larger and larger energies. The fraction of injected particles is $\lesssim 0.5\%$ for electrons and $\approx 1\%$ for protons, and the corresponding energy efficiencies are $\lesssim 2\%$ and $\approx 10\%$, respectively. The extent of the nonthermal tail is sensitive to the Alfv\'{e}n Mach number; when $\mathcal{M}_{\rm A}\lesssim 10$, the nonthermal electron distribution exhibits minimal growth beyond the average momentum of the downstream thermal protons, independently of the proton-to-electron mass ratio. Acceleration is slow for shocks with low sonic Mach numbers, yet nonthermal electrons still achieve momenta exceeding the downstream thermal proton momentum when the shock Alfv\'{e}n Mach number is large enough. We provide simulation-based parametrizations of the transition from thermal to nonthermal distribution in the downstream (found at a momentum around $p_{\rm i,e}/m_{\rm i}v_{\rm sh} \approx 3\sqrt{m_{\rm i,e}/m_{\rm i}}$), as well as the ratio of nonthermal electron to proton number density. The results are applicable to many different environments and are important for modeling shock-powered nonthermal radiation.
准平行非相对论冲击下的电子加速:一维动力学调查
我们对准平行非相对论冲击的一维动力学粒子在胞模拟进行了调查,以确定有利于电子加速的环境。我们探索了前所未有的冲击速度范围$v_{\rm sh}\approx 0.067-0.267\,c$、Alfv\'{e}n 马赫数$\mathcal{M}_{\rmA} = 5-40$、声波马赫数$\mathcal{M}_{\rm s} = 5-160$,以及质子-电子质量比$m_{\rm i}/m_{\rm e}= 16-1836$。我们发现,高Alfv\'{e}n 马赫数冲击可以将其动能的很大一部分导入非热粒子、自持磁湍流并加速到越来越大的能量。电子和质子的注入粒子比例分别为0.5%和1%,相应的能量效率分别为2%和10%。非热尾的范围对Alfv\'{e}nMach数很敏感;当$\mathcal{M}_\{rm A}\lesssim 10$时,非热电子分布的增长极小,超过了下游热质子的平均动量,与质子-电子质量比无关。对于低声速马赫数的冲击来说,加速是缓慢的,然而当冲击的Alfv\'{e}n 马赫数足够大时,非热电子仍然可以获得超过下游热质子动量的动量。我们提供了下游从热分布向非热分布过渡的基于模拟的参数(发现的动量约为 $p_{\rm i,e}/m_{\rmi}v_{\rm sh}\约3(sqrt{m_{rm i,e}/m_{\rm i}}$),以及非热电子与质子数量密度之比。这些结果适用于许多不同的环境,对于模拟冲击力非热辐射非常重要。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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