Electron Temperature Gradient Scale at Collisionless Shocks

Steven J. Schwartz, Edmund Henley, Jeremy Mitchell, and Vladimir Krasnoselskikh
Phys. Rev. Lett. 107, 215002 – Published 14 November 2011

Abstract

Shock waves are ubiquitous in space and astrophysics. They transform directed flow energy into thermal energy and accelerate energetic particles. The energy repartition is a multiscale process related to the spatial and temporal structure of the electromagnetic fields within the shock layer. While large scale features of ion heating are known, the electron heating and smaller scale fields remain poorly understood. We determine for the first time the scale of the electron temperature gradient via electron distributions measured in situ by the Cluster spacecraft. Half of the electron heating coincides with a narrow layer several electron inertial lengths (c/ωpe) thick. Consequently, the nonlinear steepening is limited by wave dispersion. The dc electric field must also vary over these small scales, strongly influencing the efficiency of shocks as cosmic ray accelerators.

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  • Received 29 June 2011

DOI:https://doi.org/10.1103/PhysRevLett.107.215002

© 2011 American Physical Society

Authors & Affiliations

Steven J. Schwartz*, Edmund Henley, and Jeremy Mitchell

  • Blackett Laboratory, Imperial College London, South Kensington, London SW7 2AZ, United Kingdom

Vladimir Krasnoselskikh

  • Laboratoire de Physique et Chimie de l’Environnement et de l’Espace, CNRS, Orléans, France

  • *s.schwartz@imperial.ac.uk

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Issue

Vol. 107, Iss. 21 — 18 November 2011

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