2013MNRAS.436..294B


Query : 2013MNRAS.436..294B

2013MNRAS.436..294B - Mon. Not. R. Astron. Soc., 436, 294-303 (2013/November-3)

Magnetic field amplification by cosmic ray-driven turbulence - I. Isotropic CR diffusion.

BRUGGEN M.

Abstract (from CDS):

We have performed magnetohydrodynamical simulations to study the amplification of magnetic fields in the precursors of shock waves. Strong magnetic fields are required in the precursors of the strong shocks that occur in supernova remnants. Observations also suggest that magnetic field amplification takes place in the weak shocks that occur in galaxy clusters and that produce the so-called radio relics. Here, we extend the study of magnetic field amplification by cosmic ray-driven turbulence to weak shocks. The amplification is driven by turbulence that is produced by the cosmic ray pressure acting on the density inhomogeneities in the upstream fluid. The clumping that has been inferred from X-ray data for the outskirts of galaxy clusters could provide some of the seed inhomogeneities. Magnetic field power spectra and Faraday maps are produced. Furthermore, we investigate how the synchrotron emission in the shock precursor can be used to verify the existence of this instability and constrain essential plasma parameters.

Abstract Copyright: © 2013 The Author Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): acceleration of particles - magnetic fields - shock waves - turbulence - ISM: supernova remnants - galaxies: clusters: intracluster medium

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
2 ACO 521 ClG 04 54 08.6 -10 14 39           ~ 279 0
3 ACO 754 ClG 09 09 14.8 -09 40 35           ~ 695 1
4 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
5 ACO 3667 ClG 20 12 33.68 -56 50 26.3           ~ 676 1
6 CIZA J2242.8+5301 ClG 22 42 53.0 +53 01 05           ~ 228 0

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