2004
DOI: 10.1103/physreve.69.016401
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Eigenmodes and growth rates of relativistic current filamentation instability in a collisional plasma

Abstract: I theoretically found eigenmodes and growth rates of relativistic current filamentation instability in collisional regimes, deriving a generalized dispersion relation from self-consistent beam-Maxwell equations. For symmetrically counterstreaming, fully relativistic electron currents, the collisional coupling between electrons and ions creates the unstable modes of growing oscillation and wave, which stand out for long-wavelength perturbations. In the stronger collisional regime, the growing oscillatory mode t… Show more

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Cited by 61 publications
(49 citation statements)
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References 46 publications
(84 reference statements)
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“…156,217 The simplicity of the Krook approach makes it widely employed in spite of its known drawbacks ͑no relaxation to a Maxwellian, nonconservation of particle number, etc.͒. More elaborate treatments for the filamentation 219 155,217,222 others find they only modify the existing collisionless unstable branch. A general trend, observed regardless of the number of branches, is that collisions tend to generate larger filaments by displacing the fastest growing filamentation modes toward the lower k's.…”
Section: -29mentioning
confidence: 99%
“…156,217 The simplicity of the Krook approach makes it widely employed in spite of its known drawbacks ͑no relaxation to a Maxwellian, nonconservation of particle number, etc.͒. More elaborate treatments for the filamentation 219 155,217,222 others find they only modify the existing collisionless unstable branch. A general trend, observed regardless of the number of branches, is that collisions tend to generate larger filaments by displacing the fastest growing filamentation modes toward the lower k's.…”
Section: -29mentioning
confidence: 99%
“…The role of collisions on the instability growth rates in the regime of interest for FI has been recently addressed analytically by a linear fluid normal mode analysis in Ref. [12] and by a linear and quasilinear kinetic approach in the limit of purely transverse modes in Ref. [13].…”
mentioning
confidence: 99%
“…Setting then ∇P i = 3k B T i ∇n i [12,22] if dealing only with electronic motion, one only needs to add to the notebook entries 4 and 5 the terms (i 2 = −1)…”
Section: Comments and Conclusionmentioning
confidence: 99%