2019A&A...622A..20H


Query : 2019A&A...622A..20H

2019A&A...622A..20H - Astronomy and Astrophysics, volume 622A, 20-20 (2019/2-1)

Radio observations of the merging galaxy cluster Abell 520.

HOANG D.N., SHIMWELL T.W., VAN WEEREN R.J., BRUNETTI G., ROTTGERING H.J.A., ANDRADE-SANTOS F., BOTTEON A., BRUGGEN M., CASSANO R., DRABENT A., DE GASPERIN F., HOEFT M., INTEMA H.T., RAFFERTY D.A., SHWETA A. and STROE A.

Abstract (from CDS):


Context. Extended synchrotron radio sources are often observed in merging galaxy clusters. Studies of the extended emission help us to understand the mechanisms in which the radio emitting particles gain their relativistic energies.
Aims. We examine the possible acceleration mechanisms of the relativistic particles that are responsible for the extended radio emission in the merging galaxy cluster Abell 520.
Methods. We performed new 145 MHz observations with the LOw Frequency ARay (LOFAR) and combined these with archival Giant Metrewave Radio Telescope (GMRT) 323 MHz and Very Large Array (VLA) 1.5GHz data to study the morphological and spectral properties of extended cluster emission. The observational properties are discussed in the framework of particle acceleration models associated with cluster merger turbulence and shocks.
Results. In Abell 520, we confirm the presence of extended (760x950kpc2) synchrotron radio emission that has been classified as a radio halo. The comparison between the radio and X-ray brightness suggests that the halo might originate in a cocoon rather than from the central X-ray bright regions of the cluster. The halo spectrum is roughly uniform on the scale of 66kpc. There is a hint of spectral steepening from the SW edge towards the cluster centre. Assuming diffusive shock acceleration (DSA), the radio data are suggestive of a shock Mach number of MSW=2.6–0.2+0.3 that is consistent with the X-ray derived estimates. This is in agreement with the scenario in which relativistic electrons in the SW radio edge gain their energies at the shock front via acceleration of either thermal or fossil electrons. We do not detect extended radio emission ahead of the SW shock that is predicted if the emission is the result of adiabatic compression. An X-ray surface brightness discontinuity is detected towards the NE region that may be a counter shock of Mach number MNEX=1.52±0.05. This is lower than the value predicted from the radio emission which, assuming DSA, is consistent with MNE=2.1±0.2.
Conclusions. Our observations indicate that the radio emission in the SW of Abell 520 is likely effected by the prominent X-ray detected shock in which radio emitting particles are (re-)accelerated through the Fermi-I mechanism. The NE X-ray discontinuity that is approximately collocated with an edge in the radio emission hints at the presence of a counter shock.

Abstract Copyright: © ESO 2019

Journal keyword(s): acceleration of particles - galaxies: clusters: individual: Abell 520 - galaxies: clusters: intracluster medium - large-scale structure of Universe

Simbad objects: 13

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Number of rows : 13
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 ACO 115 ClG 00 55 59.5 +26 19 14           ~ 270 1
2 ACT-CL J0102-4915 ClG 01 02 52.50 -49 14 58.0           ~ 229 0
3 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2815 2
4 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 436 0
5 QSO J0459+0229 QSO 04 59 52.05066296 +02 29 31.1765162   18.2 19     ~ 163 1
6 ICRF J050321.1+020304 Sy2 05 03 21.19716454 +02 03 04.6765714   22.500 21.350 20.682   ~ 188 1
7 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 851 1
8 M 1 SNR 05 34 30.9 +22 00 53           ~ 6191 1
9 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1493 1
10 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 437 0
11 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
12 ACO 2146 ClG 15 56 04.7 +66 20 24           ~ 176 0
13 3C 461 BL? 23 23 24.000 +58 48 54.00     14.30     ~ 2791 1

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