Fast dissipation of Colliding Alfvén Waves in a Magnetically Dominated Plasma
arXiv:2103.05700 · doi:10.3847/1538-4357/abfe5f
Abstract
Magnetic energy around compact objects often dominates over plasma rest mass, and its dissipation can power the object luminosity. We describe a dissipation mechanism which works faster than magnetic reconnection. The mechanism involves two strong Alfvén waves with anti-aligned magnetic fields and that propagate in opposite directions along background magnetic field and collide. The collision forms a thin current sheet perpendicular to , which absorbs the incoming waves. The current sheet is sustained by electric field breaking the magnetohydrodynamic condition and accelerating particles to high energies. We demonstrate this mechanism with kinetic plasma simulations using a simple setup of two symmetric plane waves with amplitude propagating in a uniform . The mechanism is activated when . It dissipates a large fraction of the wave energy, , reaching when . The plane geometry allows one to see the dissipation process in a one-dimensional simulation. We also perform two-dimensional simulations, enabling spontaneous breaking of the plane symmetry by the tearing instability of the current sheet. At moderate of main interest the tearing instability is suppressed. Dissipation transitions to normal, slower, magnetic reconnection at . The fast dissipation described in this paper may occur in various objects with perturbed magnetic fields, including magnetars, jets from accreting black holes, and pulsar wind nebulae.
arXiv comment12 pages, 10 figures, submitted to ApJ
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- Exact nonlinear solutions for three-dimensional Alfvén-wave packets in relativistic magnetohydrodynamics
- Breakdown of force-free electrodynamics in electric zones
- Particle acceleration by counter-propagating circularly polarized Alfvén waves
- Heating of Magnetically Dominated Plasma by Alfvén-Wave Turbulence