2021MNRAS.500..795D


Query : 2021MNRAS.500..795D

2021MNRAS.500..795D - Mon. Not. R. Astron. Soc., 500, 795-816 (2021/January-1)

Morphology of radio relics - I. What causes the substructure of synchrotron emission?

DOMINGUEZ-FERNANDEZ P., BRUGGEN M., VAZZA F., BANDA-BARRAGAN W.E., RAJPUROHIT K., MIGNONE A., MUKHERJEE D. and VAIDYA B.

Abstract (from CDS):

High-resolution radio observations of cluster radio relics often show complex spatial and spectral features. However, itis not clear what these features reveal about the underlying magnetic field properties. We performed three-dimensionalmagnetohydrodynamical simulations of merger shock waves propagating through a magnetized, turbulent intracluster medium.Our model includes the diffusive shock acceleration (DSA) of cosmic ray electrons, their spatial advection and energy lossesat run-time. With this set-up we can investigate the relation between radio substructure and pre-shock plasma conditions in thehost cluster. We find that upstream turbulence plays a major role in shaping the properties of radio relics produced downstream.Within the assumption of DSA, we can reproduce the observed discrepancy between the X-ray derived Mach number of shocks,and the Mach number inferred from radio spectra. Our simulated spectral index maps and profiles across the radio relic alsosuggest that the standard deviation of the upstream magnetic field must be relatively small (σB ≤ 1 µG) in order to reproduceobservations and therefore radio relics can potentially constrain the distribution of magnetic fields in galaxy clusters outskirts.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): acceleration of particles - shock waves - methods: numerical - galaxies: clusters: intracluster medium

Simbad objects: 3

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Number of rows : 3
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 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
2 ClG J0603.3+4214 ClG 06 03.3 +42 14           ~ 141 0
3 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 511 0

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