Ultra-long simulations of collisionless relativistic shocks in front-comoving frame: evidence for a steady state and its properties

arXiv:2607.14235 · astro-ph.HE, physics.plasm-ph · Submitted 2026-07-15 · Read on arXiv

Mikhail Garasev, Evgeny Derishev

astro-ph.HE, physics.plasm-ph

Submitted: 2026-07-15

Comments: 16 pages, 12 figures

License: http://creativecommons.org/licenses/by/4.0/

The gist: We present a series of unprecedently long 2D3V PIC simulations of unmagnetized relativistic e-e+ -pair shocks performed in a front-comoving frame.

Terminology

Abstract

We present a series of unprecedently long 2D3V PIC simulations of unmagnetized relativistic e-e+ -pair shocks performed in a front-comoving frame. By implementing a moving-wall boundary condition in the downstream together with continuous injection at the upstream boundary, we maintain a fixed simulation domain size, opening the way to perform substantially longer simulations. Our longest runs extend beyond 100000, omega p-1, exceeding the duration of the previously published simulations by a factor of several. Across a diverse set of simulations -- varying upstream/downstream lengths, transverse sizes, and particle-per-cell counts -- we find strong evidence that the shock approaches an asymptotic, time-independent state. In the downstream region, the steady state depends only on the upstream temperature at the injection boundary and does not depend on a particular numerical realization. The upstream precursor evolves slower and retains a dependence on the simulation's upstream length, that may be of minor observational consequence, since radiation from astrophysical shocks predominantly originates from the downstream region. We also find that Fermi-type acceleration is limited in energy and a true power-law tail never forms. Another important finding is that the downstream magnetic field has a soliton-like structure, where individual magnetic domains evolve independently, each comprising a compact, highly magnetized core embedded within an extended, weakly magnetized region. The magnetic-field distribution around the centers of these spots has approximately Lorentzian profile.

Sources

Related papers