{"title":"Electron Acceleration at Quasi-parallel Non-relativistic Shocks: A 1D Kinetic Survey","authors":"Siddhartha Gupta, Damiano Caprioli, Anatoly Spitkovsky","doi":"arxiv-2408.16071","DOIUrl":null,"url":null,"abstract":"We present a survey of 1D kinetic particle-in-cell simulations of\nquasi-parallel non-relativistic shocks to identify the environments favorable\nfor electron acceleration. We explore an unprecedented range of shock speeds\n$v_{\\rm sh}\\approx 0.067-0.267\\,c$, Alfv\\'{e}n Mach numbers $\\mathcal{M}_{\\rm\nA} = 5-40$, sonic Mach numbers $\\mathcal{M}_{\\rm s} = 5-160$, as well as the\nproton-to-electron mass ratios $m_{\\rm i}/m_{\\rm e}=16-1836$. We find that high\nAlfv\\'{e}n Mach number shocks can channel a large fraction of their kinetic\nenergy into nonthermal particles, self-sustaining magnetic turbulence and\nacceleration to larger and larger energies. The fraction of injected particles\nis $\\lesssim 0.5\\%$ for electrons and $\\approx 1\\%$ for protons, and the\ncorresponding energy efficiencies are $\\lesssim 2\\%$ and $\\approx 10\\%$,\nrespectively. The extent of the nonthermal tail is sensitive to the Alfv\\'{e}n\nMach number; when $\\mathcal{M}_{\\rm A}\\lesssim 10$, the nonthermal electron\ndistribution exhibits minimal growth beyond the average momentum of the\ndownstream thermal protons, independently of the proton-to-electron mass ratio.\nAcceleration is slow for shocks with low sonic Mach numbers, yet nonthermal\nelectrons still achieve momenta exceeding the downstream thermal proton\nmomentum when the shock Alfv\\'{e}n Mach number is large enough. We provide\nsimulation-based parametrizations of the transition from thermal to nonthermal\ndistribution in the downstream (found at a momentum around $p_{\\rm i,e}/m_{\\rm\ni}v_{\\rm sh} \\approx 3\\sqrt{m_{\\rm i,e}/m_{\\rm i}}$), as well as the ratio of\nnonthermal electron to proton number density. The results are applicable to\nmany different environments and are important for modeling shock-powered\nnonthermal radiation.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"45 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Plasma Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.16071","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
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.