2024A&A...686A..44R


Query : 2024A&A...686A..44R

2024A&A...686A..44R - Astronomy and Astrophysics, volume 686A44 (2024/6-1)

A “MeerKAT-meets-LOFAR” study of the complex multi-component (mini-)halo in the extreme sloshing cluster Abell 2142.

RISELEY C.J., BONAFEDE A., BRUNO L., BOTTEON A., ROSSETTI M., BIAVA N., BONNASSIEUX E., LOI F., VERNSTROM T. and BALBONI M.

Abstract (from CDS):

Context. Clusters of galaxies are known to be turbulent environments, whether they are merging systems where turbulence is injected via the conversion of gravitational potential energy into the intracluster medium (ICM), or whether they are relaxed systems in which small-scale core sloshing is occurring within the potential well. In many such systems, diffuse radio sources associated with the ICM are found: radio haloes and mini-haloes.
Aims. Abell 2142 is a rich cluster undergoing an extreme episode of core sloshing, which has given rise to four cold fronts and a complex multi-component radio halo. Recent work revealed that there are three primary components to the halo that spans a distance of up to around 2.4 Mpc. The underlying physics of particle acceleration on these scales is poorly explored, and requires high-quality multi-frequency data with which to perform precision spectral investigation. We aim to perform such an investigation.
Methods. We used new deep MeerKAT L-band (1283 MHz) observations in conjunction with LOFAR HBA (143 MHz) data as well as X-ray data from XMM-Newton and Chandra to study the spectrum of the halo and the connection between the thermal and non-thermal components of the ICM.
Results. We confirm the presence of the third halo component, detecting it for the first time at 1283 MHz and confirming its ultra-steep spectrum nature, as we recovered an integrated spectrum of α_H3, total_ = -1.68 ± 0.10. All halo components follow power-law spectra with increasingly steep spectra moving towards the cluster outskirts. We profiled the halo in three directions, finding evidence of asymmetry and spectral steepening along an axis perpendicular to the main axis of the cluster. Our investigation of the thermal non-thermal connection shows sub-linear correlations that are steeper at 1283 MHz than 143 MHz, and we find evidence of different connections in different components of the halo. In particular, we find both a moderate anti-correlation (H1, the core) and positive correlation (H2, the ridge) between the radio spectral index and X-ray temperature.
Conclusions. Our results are broadly consistent with an interpretation of turbulent (re-)acceleration following an historic minor cluster merger scenario in which we must invoke some inhomogeneities. However, the anti-correlation between the radio spectral index and X-ray temperature in the cluster core is more challenging to explain; the presence of three cold fronts and a generally lower temperature may provide the foundations of an explanation, but detailed modelling is required to study this further.

Abstract Copyright: © The Authors 2024

Journal keyword(s): galaxies: clusters: general - galaxies: clusters: intracluster medium - galaxies: clusters: individual: Abell 2142 - radio continuum: general

VizieR on-line data: <Available at CDS (J/A+A/686/A44): list.dat fits/*>

Simbad objects: 22

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Number of rows : 22
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 0217+70 ClG 02 17 00.0 +70 36 00           ~ 40 0
3 ACO 521 ClG 04 54 08.6 -10 14 39           ~ 279 0
4 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 511 0
5 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 456 0
6 ACO 3558 ClG 13 28 03.2 -31 31 35           ~ 476 2
7 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
8 ZwCl 1455+2232 ClG 14 57 15.2 +22 20 30     18.62 20.04   ~ 309 0
9 NAME CrB Supercluster SCG 15 25 +29.5           ~ 148 0
10 2MASX J15581330+2714531 BiC 15 58 13.2945664080 +27 14 53.232436860   16.62       ~ 20 0
11 B2 1556+27 rG 15 58 14.0 +27 16 22           ~ 12 2
12 NVSS J155813+271622 rG 15 58 14.3093579688 +27 16 19.571108448   17.96       ~ 27 1
13 2MASX J15582002+2714000 BiC 15 58 20.000 +27 14 00.28   14.48       ~ 40 1
14 2MASX J15582091+2720010 BiC 15 58 20.8826270472 +27 20 01.464333504   16.07       ~ 19 0
15 ACO 2142 ClG 15 58 26.5 +27 13 52           ~ 825 0
16 LEDA 1783783 BiC 15 58 45.4271769360 +26 38 51.596598300           ~ 10 0
17 7C 1557+2712 Rad 15 59 05.2 +27 03 52           ~ 2 0
18 ICRF J160913.3+264129 Sy2 16 09 13.3196 +26 41 29.042   19       ~ 249 1
19 ACO 2256 ClG 17 03 37.5 +78 37 23           ~ 928 1
20 ACO 2255 ClG 17 12 56.0 +64 04 06           ~ 605 0
21 ClG J1720+2638 ClG 17 20 09.6 +26 37 35           ~ 284 0
22 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1332 2

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