The radiative signature of Fermi acceleration at relativistic shocks

The first-order Fermi process at relativistic shocks requires the generation of strong turbulence in the vicinity of the shock front. Recent particle in cell simulations have demonstrated that this mechanism can be studied self-consistently at weakly magnetised shocks. In this case, strong electroma...

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Main Authors: Reville, B, Kirk, J
Format: Journal article
Language:English
Published: 2010
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author Reville, B
Kirk, J
author_facet Reville, B
Kirk, J
author_sort Reville, B
collection OXFORD
description The first-order Fermi process at relativistic shocks requires the generation of strong turbulence in the vicinity of the shock front. Recent particle in cell simulations have demonstrated that this mechanism can be studied self-consistently at weakly magnetised shocks. In this case, strong electromagnetic fields are generated on length-scales comparable to the plasma skin-depth. The resulting diffusion and radiation spectrum in this short-wavelength turbulence can differ significantly from the standard picture. A connection between these two processes can be found which predicts an upper limit to the maximum photon energy that can be produced via synchrotron type radiation at a relativistic shock.
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spelling oxford-uuid:06b9b3e9-862a-4e5d-9afe-ef1ee12525042022-03-26T09:03:56ZThe radiative signature of Fermi acceleration at relativistic shocksJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:06b9b3e9-862a-4e5d-9afe-ef1ee1252504EnglishSymplectic Elements at Oxford2010Reville, BKirk, JThe first-order Fermi process at relativistic shocks requires the generation of strong turbulence in the vicinity of the shock front. Recent particle in cell simulations have demonstrated that this mechanism can be studied self-consistently at weakly magnetised shocks. In this case, strong electromagnetic fields are generated on length-scales comparable to the plasma skin-depth. The resulting diffusion and radiation spectrum in this short-wavelength turbulence can differ significantly from the standard picture. A connection between these two processes can be found which predicts an upper limit to the maximum photon energy that can be produced via synchrotron type radiation at a relativistic shock.
spellingShingle Reville, B
Kirk, J
The radiative signature of Fermi acceleration at relativistic shocks
title The radiative signature of Fermi acceleration at relativistic shocks
title_full The radiative signature of Fermi acceleration at relativistic shocks
title_fullStr The radiative signature of Fermi acceleration at relativistic shocks
title_full_unstemmed The radiative signature of Fermi acceleration at relativistic shocks
title_short The radiative signature of Fermi acceleration at relativistic shocks
title_sort radiative signature of fermi acceleration at relativistic shocks
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AT kirkj theradiativesignatureoffermiaccelerationatrelativisticshocks
AT revilleb radiativesignatureoffermiaccelerationatrelativisticshocks
AT kirkj radiativesignatureoffermiaccelerationatrelativisticshocks