Electron-ion coupling upstream of relativistic collisionless shocks

dc.creatorLyubarsky, Yuri
dc.date2006-11-01
dc.date.accessioned2026-07-07T10:40:42Z
dc.date.available2026-07-07T10:40:42Z
dc.descriptionIt is argued and demonstrated by particle-in-cell simulations that the synchrotron maser instability could develop at the front of a relativistic, magnetized shock. The instability generates strong low-frequency electromagnetic waves propagating both upstream and downstream of the shock. Upstream of the shock, these waves make electrons lag behind ions so that a longitudinal electric field arises and the electrons are accelerated up to the ion kinetic energy. Then thermalization at the shock front results in a plasma with equal temperatures of electrons and ions. Downstream of the shock, the amplitude of the maser-generated wave may exceed the strength of the shock-compressed background magnetic field. In this case the shock-accelerated particles radiate via nonlinear Compton scattering rather than via a synchrotron mechanism. The spectrum of the radiation differs, in the low-frequency band, from that of the synchrotron radiation, providing possible observational tests of the model.
dc.description22 pages, 10 figures. To appear in ApJ vol. 653
dc.identifierhttps://arxiv.org/abs/astro-ph/0611015
dc.identifierhttp://arxiv.org/abs/astro-ph/0611015
dc.identifierAstrophys.J.652:1297-1305,2006
dc.identifierdoi:10.1086/508606
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/181412
dc.subjectAstrophysics
dc.titleElectron-ion coupling upstream of relativistic collisionless shocks
dc.typetext

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