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Title: Electromagnetic waves destabilized by runaway electrons in near-critical electric fields

Abstract

Runaway electron distributions are strongly anisotropic in velocity space. This anisotropy is a source of free energy that may destabilize electromagnetic waves through a resonant interaction between the waves and the energetic electrons. In this work, we investigate the high-frequency electromagnetic waves that are destabilized by runaway electron beams when the electric field is close to the critical field for runaway acceleration. Using a runaway electron distribution appropriate for the near-critical case, we calculate the linear instability growth rate of these waves and conclude that the obliquely propagating whistler waves are most unstable. We show that the frequencies, wave numbers, and propagation angles of the most unstable waves depend strongly on the magnetic field. Taking into account collisional and convective damping of the waves, we determine the number density of runaways that is required to destabilize the waves and show its parametric dependences.

Authors:
;  [1];  [2]
  1. Department of Nuclear Techniques, Budapest University of Technology and Economics, Association EURATOM, H-1111 Budapest (Hungary)
  2. Department of Applied Physics, Nuclear Engineering, Chalmers University of Technology and Euratom-VR Association, Goeteborg (Sweden)
Publication Date:
OSTI Identifier:
22113329
Resource Type:
Journal Article
Resource Relation:
Journal Name: Physics of Plasmas; Journal Volume: 20; Journal Issue: 1; Other Information: (c) 2013 EURATOM; Country of input: International Atomic Energy Agency (IAEA)
Country of Publication:
United States
Language:
English
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; ACCELERATION; ANISOTROPY; COLLISIONS; CRITICAL FIELD; ELECTRIC FIELDS; FREE ENERGY; INSTABILITY GROWTH RATES; INTERACTIONS; PLASMA; PLASMA DENSITY; PLASMA INSTABILITY; RUNAWAY ELECTRONS; TAIL ELECTRONS

Citation Formats

Komar, A., Pokol, G. I., and Fueloep, T. Electromagnetic waves destabilized by runaway electrons in near-critical electric fields. United States: N. p., 2013. Web. doi:10.1063/1.4776666.
Komar, A., Pokol, G. I., & Fueloep, T. Electromagnetic waves destabilized by runaway electrons in near-critical electric fields. United States. doi:10.1063/1.4776666.
Komar, A., Pokol, G. I., and Fueloep, T. Tue . "Electromagnetic waves destabilized by runaway electrons in near-critical electric fields". United States. doi:10.1063/1.4776666.
@article{osti_22113329,
title = {Electromagnetic waves destabilized by runaway electrons in near-critical electric fields},
author = {Komar, A. and Pokol, G. I. and Fueloep, T.},
abstractNote = {Runaway electron distributions are strongly anisotropic in velocity space. This anisotropy is a source of free energy that may destabilize electromagnetic waves through a resonant interaction between the waves and the energetic electrons. In this work, we investigate the high-frequency electromagnetic waves that are destabilized by runaway electron beams when the electric field is close to the critical field for runaway acceleration. Using a runaway electron distribution appropriate for the near-critical case, we calculate the linear instability growth rate of these waves and conclude that the obliquely propagating whistler waves are most unstable. We show that the frequencies, wave numbers, and propagation angles of the most unstable waves depend strongly on the magnetic field. Taking into account collisional and convective damping of the waves, we determine the number density of runaways that is required to destabilize the waves and show its parametric dependences.},
doi = {10.1063/1.4776666},
journal = {Physics of Plasmas},
number = 1,
volume = 20,
place = {United States},
year = {Tue Jan 15 00:00:00 EST 2013},
month = {Tue Jan 15 00:00:00 EST 2013}
}
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