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Particle Acceleration, Magnetic Field Generation, and Emission in Relativistic Shocks
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Particle Acceleration, Magnetic Field
Generation, and Emission in Relativistic
Shocks
K.-I. Nishikawa, a P. Hardee, b C. B. Hededal, c G. Richardson, d
R. Preece, e H. Sol, f and G. J. Fishman g
aNational Space Science and Technology Center, Huntsville, AL 35805 USA
bDepartment of Physics and Astronomy, The University of Alabama, Tuscaloosa,
AL 35487 USA
cNiels Bohr Institute, Department of Astrophysics, Juliane Maries Vej30, 2100
K?benhavn ?, Denmark
dDepartment of Mechanical and Aerospace Engineering University of Alabama in
Huntsville Huntsville, AL 35899 USA
eDepartment of Physics, University of Alabama in Huntsville, Huntsville, AL
35899 and National Space Science and Technology Center, Huntsville, AL 35805
USA
fLUTH, Observatore de Paris-Meudon, 5 place Jules Jansen 92195 Meudon
Cedex, France
gNASA-Marshall Space Flight Center,
National Space Science and Technology Center, Huntsville, AL 35805 USA
Abstract
Shock acceleration is a ubiquitous phenomenon in astrophysical plasmas. Plasma
waves and their associated instabilities (e.g., Buneman,Weibel and other two-stream
instabilities) created in collisionless shocks are responsible for particle (electron,
positron, and ion) acceleration. Using a 3-D relativistic electromagnetic particle
(REMP) code, we have investigated particle acceleration associated with a rela-
tivistic jet front propagating into an ambient plasma. We find small differences in
the results for no ambient and modest ambient magnetic fields. Simulations show
that the Weibel instability created in the collisionless shock front accelerates jet and
ambient particles both perpendicular and parallel to the jet propagation direction.
The small scale magnetic field structure generated by the Weibel instability is ap-
propriate to the generation of “jitter” radiation from deflected electrons (positrons)
as opposed to synchrotron radiation. The jitter radiation resulting from small scale
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