Fermi acceleration in relativistic collisionless plasma shocks correlates with anisotropic energy gains

Fuente: arXiv
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Autores principales: Rajawat, Roopendra Singh, Khudik, Vladimir, Shvets, Gennady
Formato: Preprint
Publicado: 2021
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author Rajawat, Roopendra Singh
Khudik, Vladimir
Shvets, Gennady
author_facet Rajawat, Roopendra Singh
Khudik, Vladimir
Shvets, Gennady
contents Collisionless shocks generated by two colliding relativistic electron-positron plasma shells are studied using particle-in-cell (PIC) simulations. Shocks are mediated by the Weibel instability (WI), and the kinetic energy of the fastest accelerated particles is found to be anisotropically modified by WI-induced electric fields. Specifically, we show that all particles interacting with the shock bifurcate into two groups based on their final relativistic Lorentz factor $γ$: slow ($γ< γ_{bf}$) and fast ($γ> γ_{bf}$), where $γ_{bf}$ is the bifurcation Lorentz factor that was found to be approximately twice the initial (upstream) Lorentz factor $γ_0$. We have found that the energies of the slow particles are equally affected by the longitudinal and transverse components of the shock electric field, whereas the fast particles are primarily accelerated by the transverse field component.
format Preprint
id arxiv_https___arxiv_org_abs_2102_11975
institution arXiv
publishDate 2021
record_format arxiv
spellingShingle Fermi acceleration in relativistic collisionless plasma shocks correlates with anisotropic energy gains
Rajawat, Roopendra Singh
Khudik, Vladimir
Shvets, Gennady
Plasma Physics
High Energy Astrophysical Phenomena
Collisionless shocks generated by two colliding relativistic electron-positron plasma shells are studied using particle-in-cell (PIC) simulations. Shocks are mediated by the Weibel instability (WI), and the kinetic energy of the fastest accelerated particles is found to be anisotropically modified by WI-induced electric fields. Specifically, we show that all particles interacting with the shock bifurcate into two groups based on their final relativistic Lorentz factor $γ$: slow ($γ< γ_{bf}$) and fast ($γ> γ_{bf}$), where $γ_{bf}$ is the bifurcation Lorentz factor that was found to be approximately twice the initial (upstream) Lorentz factor $γ_0$. We have found that the energies of the slow particles are equally affected by the longitudinal and transverse components of the shock electric field, whereas the fast particles are primarily accelerated by the transverse field component.
title Fermi acceleration in relativistic collisionless plasma shocks correlates with anisotropic energy gains
topic Plasma Physics
High Energy Astrophysical Phenomena
url https://arxiv.org/abs/2102.11975