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Preferential positron heating and acceleration by synchrotron maser instabilities in relativistic positron–electron–proton plasmas

Phys. Fluids B 3, 818 (1991); doi:10.1063/1.859877

Issue Date: March 1991

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Masahiro Hoshino and Jonathan Arons
Institute of Geophysics and Planetary Physics, Lawrence Livermore National Laboratory, University of California, Livermore, California 94550
In this paper, a new process of the preferential strong heating of positrons through the ion synchrotron maser instability in positron–electron–proton (e+ep+) magnetized plasmas is studied, using particle-in-cell simulations. It is found that the positrons form a nonthermal power-law-like energy distribution through their gyroresonant interaction with the extraordinary modes emitted by the ions. This process may be important for the shock excitation of the nonthermal synchrotron radiation observed from astrophysical systems powered by relativistic outflows from compact central objects (e.g., supernova remnants powered by pulsars and jets from active galactic nuclei). When the initial particle distributions are cold rings in momentum space for all three species, there are two stages of instability. The electrons and positrons first thermalize through the emission of collective extraordinary modes. This phase is followed by the emission of collective proton synchrotron radiation, a process with a slower growth rate than the maser in the e and e+. When the gyrational energy density of the protons exceeds that of the e+, a significant amount of energy can be transferred to the positrons through resonant interaction between the e+, which gyrate in the same sense as the p+, and the elliptically polarized proton synchrotron modes whose frequency is at high harmonics of the fundamental proton gyrofrequency and whose electric field vector has the same sense of rotation as the protons and positrons. The final spectrum of the positrons has a power-law distribution in energy space: The number of positrons with relativistic energy between E and E+dE is N(E)dE[proportional]E−2. The electrons, which have the opposite sense of gyromotion to the protons, are not accelerated and retain the relativistic Maxwellian distribution that results from the synchrotron maser instability in the pairs alone. A brief discussion of the relevance of these results to the structure of collisionless relativistic shock waves in astrophysical sources of synchrotron radiation is presented. Physics of Fluids B: Plasma Physics is copyrighted by The American Institute of Physics.
History: Received 31 August 1990; accepted 15 November 1990
Permalink: http://dx.doi.org/10.1063/1.859877
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KEYWORDS and PACS

Keywords
PACS
  • 52.35.Qz
    The physics of plasmas and electric discharges Waves, oscillations, and instabilities in plasma Plasma microinstabilities (ion-acoustic, two-stream, loss-cone, beam-plasma, drift, ion- or electron-cyclotron, etc.)
  • 52.65.+z
    The physics of plasmas and electric discharges Plasma simulation (e.g., particle orbit and trajectory, MHD equilibrium and stability, initial value computation, and heat transport models; Monte Carlo methods)
  • 52.60.+h
    The physics of plasmas and electric discharges Relativistic plasma
  • 98.40.Ne
    Stellar systems; galactic and extragalactic objects and systems; the Universe Interstellar matter and nebulae Supernova remnants
  • YEAR: 1990-91

PUBLICATION DATA

ISSN:
0899-8221 (print)   1089-7674 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (18)

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