Cosmic-Ray Drag and Damping of Compressive Turbulence

While it is well known that cosmic rays (CRs) can gain energy from turbulence via second-order Fermi acceleration, how this energy transfer affects the turbulent cascade remains largely unexplored. Here, we show that damping and steepening of the compressive turbulent power spectrum are expected onc...

Full description

Bibliographic Details
Main Authors: Chad Bustard, S. Peng Oh
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/aceef9
_version_ 1827814346796826624
author Chad Bustard
S. Peng Oh
author_facet Chad Bustard
S. Peng Oh
author_sort Chad Bustard
collection DOAJ
description While it is well known that cosmic rays (CRs) can gain energy from turbulence via second-order Fermi acceleration, how this energy transfer affects the turbulent cascade remains largely unexplored. Here, we show that damping and steepening of the compressive turbulent power spectrum are expected once the damping time ${t}_{\mathrm{damp}}\sim \rho {v}^{2}/{\dot{E}}_{\mathrm{CR}}\propto {E}_{\mathrm{CR}}^{-1}$ becomes comparable to the turbulent cascade time. Magnetohydrodynamic simulations of stirred compressive turbulence in a gas-CR fluid with diffusive CR transport show clear imprints of CR-induced damping, saturating at ${\dot{E}}_{\mathrm{CR}}\sim \tilde{\epsilon }$ , where $\tilde{\epsilon }$ is the turbulent energy input rate. In that case, almost all of the energy in large-scale motions is absorbed by CRs and does not cascade down to grid scale. Through a Hodge–Helmholtz decomposition, we confirm that purely compressive forcing can generate significant solenoidal motions, and we find preferential CR damping of the compressive component in simulations with diffusion and streaming, rendering small-scale turbulence largely solenoidal, with implications for thermal instability and proposed resonant scattering of E ≳ 300 GeV CRs by fast modes. When CR transport is streaming dominated, CRs also damp large-scale motions, with kinetic energy reduced by up to 1 order of magnitude in realistic E _CR ∼ E _g scenarios, but turbulence (with a reduced amplitude) still cascades down to small scales with the same power spectrum. Such large-scale damping implies that turbulent velocities obtained from the observed velocity dispersion may significantly underestimate turbulent forcing rates, i.e., $\tilde{\epsilon }\gg \rho {v}^{3}/L$ .
first_indexed 2024-03-11T23:45:13Z
format Article
id doaj.art-a72b5615453f42cfb5a9c91b31efe197
institution Directory Open Access Journal
issn 1538-4357
language English
last_indexed 2024-03-11T23:45:13Z
publishDate 2023-01-01
publisher IOP Publishing
record_format Article
series The Astrophysical Journal
spelling doaj.art-a72b5615453f42cfb5a9c91b31efe1972023-09-19T12:19:19ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-0195516410.3847/1538-4357/aceef9Cosmic-Ray Drag and Damping of Compressive TurbulenceChad Bustard0https://orcid.org/0000-0002-8366-2143S. Peng Oh1https://orcid.org/0000-0002-1013-4657Kavli Institute for Theoretical Physics, University of California—Santa Barbara , Kohn Hall, Santa Barbara, CA 93107, USA ; bustard@ucsb.eduDepartment of Physics, University of California—Santa Barbara , Broida Hall, Santa Barbara, CA 93106, USAWhile it is well known that cosmic rays (CRs) can gain energy from turbulence via second-order Fermi acceleration, how this energy transfer affects the turbulent cascade remains largely unexplored. Here, we show that damping and steepening of the compressive turbulent power spectrum are expected once the damping time ${t}_{\mathrm{damp}}\sim \rho {v}^{2}/{\dot{E}}_{\mathrm{CR}}\propto {E}_{\mathrm{CR}}^{-1}$ becomes comparable to the turbulent cascade time. Magnetohydrodynamic simulations of stirred compressive turbulence in a gas-CR fluid with diffusive CR transport show clear imprints of CR-induced damping, saturating at ${\dot{E}}_{\mathrm{CR}}\sim \tilde{\epsilon }$ , where $\tilde{\epsilon }$ is the turbulent energy input rate. In that case, almost all of the energy in large-scale motions is absorbed by CRs and does not cascade down to grid scale. Through a Hodge–Helmholtz decomposition, we confirm that purely compressive forcing can generate significant solenoidal motions, and we find preferential CR damping of the compressive component in simulations with diffusion and streaming, rendering small-scale turbulence largely solenoidal, with implications for thermal instability and proposed resonant scattering of E ≳ 300 GeV CRs by fast modes. When CR transport is streaming dominated, CRs also damp large-scale motions, with kinetic energy reduced by up to 1 order of magnitude in realistic E _CR ∼ E _g scenarios, but turbulence (with a reduced amplitude) still cascades down to small scales with the same power spectrum. Such large-scale damping implies that turbulent velocities obtained from the observed velocity dispersion may significantly underestimate turbulent forcing rates, i.e., $\tilde{\epsilon }\gg \rho {v}^{3}/L$ .https://doi.org/10.3847/1538-4357/aceef9Cosmic raysMagnetohydrodynamicsPlasma astrophysicsCircumgalactic mediumInterstellar medium
spellingShingle Chad Bustard
S. Peng Oh
Cosmic-Ray Drag and Damping of Compressive Turbulence
The Astrophysical Journal
Cosmic rays
Magnetohydrodynamics
Plasma astrophysics
Circumgalactic medium
Interstellar medium
title Cosmic-Ray Drag and Damping of Compressive Turbulence
title_full Cosmic-Ray Drag and Damping of Compressive Turbulence
title_fullStr Cosmic-Ray Drag and Damping of Compressive Turbulence
title_full_unstemmed Cosmic-Ray Drag and Damping of Compressive Turbulence
title_short Cosmic-Ray Drag and Damping of Compressive Turbulence
title_sort cosmic ray drag and damping of compressive turbulence
topic Cosmic rays
Magnetohydrodynamics
Plasma astrophysics
Circumgalactic medium
Interstellar medium
url https://doi.org/10.3847/1538-4357/aceef9
work_keys_str_mv AT chadbustard cosmicraydraganddampingofcompressiveturbulence
AT spengoh cosmicraydraganddampingofcompressiveturbulence