{"title":"准平行非相对论冲击下的电子加速:一维动力学调查","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":"{\"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}","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}
Electron Acceleration at Quasi-parallel Non-relativistic Shocks: A 1D Kinetic Survey
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.