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Kinetic Simulations of the Filamentation Instability in Pair Plasmas

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arxiv 2304.03577 v1 pith:NC2G6ME4 submitted 2023-04-07 astro-ph.HE physics.plasm-ph

classification astro-ph.HEphysics.plasm-ph
keywords mergingnonlinearplasmassimulationsaffectdensityelectromagneticfilamentation
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The nonlinear interaction between electromagnetic waves and plasmas attracts significant attention in astrophysics because it can affect the propagation of Fast Radio Bursts (FRBs) -- luminous millisecond-duration pulses detected at radio frequency. The filamentation instability (FI) -- a type of nonlinear wave-plasma interaction -- is considered to be dominant near FRB sources, and its nonlinear development may also affect the inferred dispersion measure of FRBs. In this paper, we carry out fully kinetic particle-in-cell simulations of the FI in unmagnetized pair plasmas. Our simulations show that the FI generates transverse density filaments, and that the electromagnetic wave propagates in near vacuum between them, as in a waveguide. The density filaments keep merging until force balance between the wave ponderomotive force and the plasma pressure gradient is established. We estimate the merging timescale and discuss the implications of filament merging for FRB observations.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Interaction of Strong Electromagnetic Waves with Unmagnetized Pair Plasmas

    physics.plasm-ph 2026-04 unverdicted novelty 7.0 of 10

    The propagation length of strong electromagnetic waves through unmagnetized pair plasmas scales as ε_p^{-2/3}, where ε_p combines wave strength and frequency, verified by kinetic simulations.

  2. Unified kinetic theory of induced scattering: Compton, Brillouin, and Raman processes in magnetized electron and positron pair plasma

    astro-ph.HE 2025-10 conditional novelty 6.0 of 10

    In strongly magnetized pair plasma, induced Compton and Brillouin scattering dominate in ordinary/neutral modes, while stimulated Raman scattering is enabled in a charged mode with growth rate (t_R)^-1 = a_e (omega0/o...

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