Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma

In astrophysical relativistic plasmas, Alfvénic turbulence exists across a wide range of scales. Similar to a nonrelativistic case, this turbulence can be influenced by the tearing instability. We argue that in an ultrarelativistic pair plasma the tearing effects become significant at the critical s...

Full description

Saved in:
Bibliographic Details
Main Authors: Stanislav Boldyrev, Nuno F. Loureiro
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/ada28a
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1832582739651461120
author Stanislav Boldyrev
Nuno F. Loureiro
author_facet Stanislav Boldyrev
Nuno F. Loureiro
author_sort Stanislav Boldyrev
collection DOAJ
description In astrophysical relativistic plasmas, Alfvénic turbulence exists across a wide range of scales. Similar to a nonrelativistic case, this turbulence can be influenced by the tearing instability. We argue that in an ultrarelativistic pair plasma the tearing effects become significant at the critical scale given by ${a}_{t}\sim {d}_{\mathrm{rel}}{\left({L}_{\perp }/{d}_{\mathrm{rel}}\right)}^{n/(4+5n)}$ , where L _⊥ represents the outer scale of the turbulence and d _rel the relativistic electron inertial scale. Here n = 1 corresponds to the Harris magnetic configurations, while n = 2 applies to localized (non-Harris) magnetic profiles of turbulence-generated current sheets. Below the critical scale, the energy spectrum of magnetic fluctuations steepens to W ( k ) dk ∝ k ^−(7 ^n ^+2)/3 ^n dk . However, this happens only when $\tilde{\sigma }\ll {\left({L}_{\perp }/{d}_{\mathrm{rel}}\right)}^{(2+4n)/(4+5n)}$ , where $\tilde{\sigma }$ is the magnetization parameter based on the magnetic fluctuations. If the opposite inequality holds, the Alfvénic cascade is instead affected by charge starvation at scales below ${a}_{\mathrm{ch}}\sim {d}_{\mathrm{rel}}{\left({d}_{\mathrm{rel}}/{L}_{\perp }\right)}^{1/3}{\tilde{\sigma }}^{2/3}$ , and the energy spectrum becomes steeper than W ( k ) dk ∝ k ^−3 dk . When d _rel is replaced by its nonrelativistic equivalent, our results agree with the nonrelativistic analysis of N. F. Loureiro & S. Boldyrev (2018). In the Harris case n = 1, they agree with the recent relativistic studies by I. Demidov & Y. Lyubarsky.
format Article
id doaj-art-3849b5f949ae40eca1264bb17646f977
institution Kabale University
issn 1538-4357
language English
publishDate 2025-01-01
publisher IOP Publishing
record_format Article
series The Astrophysical Journal
spelling doaj-art-3849b5f949ae40eca1264bb17646f9772025-01-29T09:57:19ZengIOP PublishingThe Astrophysical Journal1538-43572025-01-01979223210.3847/1538-4357/ada28aTearing-mediated Alfvénic Turbulence in a Relativistic PlasmaStanislav Boldyrev0https://orcid.org/0000-0001-6252-5169Nuno F. Loureiro1https://orcid.org/0000-0001-9755-6563Department of Physics, University of Wisconsin –Madison, Madison, WI 53706, USA; Space Science Institute , Boulder, CO 80301, USAPlasma Science and Fusion Center, Massachusetts Institute of Technology , Cambridge, MA 02139, USAIn astrophysical relativistic plasmas, Alfvénic turbulence exists across a wide range of scales. Similar to a nonrelativistic case, this turbulence can be influenced by the tearing instability. We argue that in an ultrarelativistic pair plasma the tearing effects become significant at the critical scale given by ${a}_{t}\sim {d}_{\mathrm{rel}}{\left({L}_{\perp }/{d}_{\mathrm{rel}}\right)}^{n/(4+5n)}$ , where L _⊥ represents the outer scale of the turbulence and d _rel the relativistic electron inertial scale. Here n = 1 corresponds to the Harris magnetic configurations, while n = 2 applies to localized (non-Harris) magnetic profiles of turbulence-generated current sheets. Below the critical scale, the energy spectrum of magnetic fluctuations steepens to W ( k ) dk ∝ k ^−(7 ^n ^+2)/3 ^n dk . However, this happens only when $\tilde{\sigma }\ll {\left({L}_{\perp }/{d}_{\mathrm{rel}}\right)}^{(2+4n)/(4+5n)}$ , where $\tilde{\sigma }$ is the magnetization parameter based on the magnetic fluctuations. If the opposite inequality holds, the Alfvénic cascade is instead affected by charge starvation at scales below ${a}_{\mathrm{ch}}\sim {d}_{\mathrm{rel}}{\left({d}_{\mathrm{rel}}/{L}_{\perp }\right)}^{1/3}{\tilde{\sigma }}^{2/3}$ , and the energy spectrum becomes steeper than W ( k ) dk ∝ k ^−3 dk . When d _rel is replaced by its nonrelativistic equivalent, our results agree with the nonrelativistic analysis of N. F. Loureiro & S. Boldyrev (2018). In the Harris case n = 1, they agree with the recent relativistic studies by I. Demidov & Y. Lyubarsky.https://doi.org/10.3847/1538-4357/ada28aPlasma astrophysicsMagnetic fields
spellingShingle Stanislav Boldyrev
Nuno F. Loureiro
Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
The Astrophysical Journal
Plasma astrophysics
Magnetic fields
title Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
title_full Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
title_fullStr Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
title_full_unstemmed Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
title_short Tearing-mediated Alfvénic Turbulence in a Relativistic Plasma
title_sort tearing mediated alfvenic turbulence in a relativistic plasma
topic Plasma astrophysics
Magnetic fields
url https://doi.org/10.3847/1538-4357/ada28a
work_keys_str_mv AT stanislavboldyrev tearingmediatedalfvenicturbulenceinarelativisticplasma
AT nunofloureiro tearingmediatedalfvenicturbulenceinarelativisticplasma