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Fast radio bursts as precursor radio emission from monster shocks

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arxiv 2407.15076 v2 pith:IQUVX6VG submitted 2024-07-21 astro-ph.HE physics.plasm-ph

classification astro-ph.HEphysics.plasm-ph
keywords fastwavemonsterprecursorradioshockburstsenergy
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abstract

It has been proposed recently that the breaking of MHD waves in the inner magnetosphere of strongly magnetized neutron stars can power different types of high-energy transients. Motivated by these considerations, we study the steepening and dissipation of a strongly magnetized fast magnetosonic wave propagating in a declining background magnetic field, by means of particle-in-cell simulations that encompass MHD scales. Our analysis confirms the formation of a monster shock as $B^2-E^2 \to 0$, that dissipates about half of the fast magnetosonic wave energy. It also reveals, for the first time, the generation of a high-frequency precursor wave by a synchrotron maser instability at the monster shock front, carrying a fraction of $\sim 10^{-3}$ of the total energy dissipated at the shock. The spectrum of the precursor wave exhibits several sharp harmonic peaks, with frequencies in the GHz band under conditions anticipated in magnetars. Such signals may appear as fast radio bursts.

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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. Relativistically Magnetized Collisionless Shocks in Pair Plasma: I. Solitons, Chaos, and Thermalization

    astro-ph.HE 2024-11 conditional novelty 7.0 of 10

    In strongly magnetized pair-plasma shocks, chaotic particle orbits inside a soliton train can fully account for dissipation and thermalization without invoking collective plasma instabilities.

  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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