2021A&A...647A..51C


Query : 2021A&A...647A..51C

2021A&A...647A..51C - Astronomy and Astrophysics, volume 647A51-51 (2021/3-1)

Radio halos in a mass-selected sample of 75 galaxy clusters. II. Statistical analysis.

CUCITI V., CASSANO R., BRUNETTI G., DALLACASA D., DE GASPERIN F., ETTORI S., GIACINTUCCI S., KALE R., PRATT G.W., VAN WEEREN R.J. and VENTURI T.

Abstract (from CDS):


Context. Many galaxy clusters host megaparsec-scale diffuse radio sources called radio halos. Their origin is tightly connected to the processes that lead to the formation of clusters themselves. In order to reveal this connection, statistical studies of the radio properties of clusters combined with their thermal properties are necessary. For this purpose, we selected a sample of galaxy clusters with M500≥6x1014M☉ and z=0.08-0.33 from the Planck Sunyaev-Zel'dovich catalogue. In Paper I (Cuciti et al., 2021A&A...647A..50C), we presented the radio and X-ray data analysis that we carried out on the clusters of this sample.
Aims. In this paper we exploit the wealth of data presented in Paper I to study the radio properties of the sample, in connection to the mass and dynamical state of clusters.
Methods. We used the dynamical information derived from the X-ray data to assess the role of mergers in the origin of radio halos. We studied the distribution of clusters in the radio power-mass diagram, the scaling between the radio luminosity of radio halos and the mass of the host clusters, and the role of dynamics in the radio luminosity and emissivity of radio halos. We measured the occurrence of radio halos as a function of the cluster mass and we compared it with the expectations of models developed in the framework of turbulent acceleration.
Results. We find that more than the 90% of radio halos are in merging clusters and that their radio power correlates with the mass of the host clusters. The correlation shows a large dispersion. Interestingly, we show that cluster dynamics contributes significantly to this dispersion, with more disturbed clusters being more radio luminous. Clusters without radio halos are generally relaxed, and the upper limits to their diffuse emission lie below the correlation. Moreover, we show that the radio emissivity of clusters exhibits an apparent bimodality, with the emissivity of radio halos being at least ∼5 times larger than the non-emission associated with more relaxed clusters. We find that the fraction of radio halos drops from ∼70% in high-mass clusters to ∼35% in the lower mass systems in the sample and we show that this result is in good agreement with the expectations from turbulent re-acceleration models.

Abstract Copyright: © ESO 2021

Journal keyword(s): galaxies: clusters: general - galaxies: clusters: intracluster medium - radiation mechanisms: non-thermal

Simbad objects: 58

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Number of rows : 58
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 2697 ClG 00 03 11.5 -06 05 30           ~ 53 0
2 ACO 2734 ClG 00 11 21.60 -28 51 16.6           ~ 156 0
3 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
4 ACO 56 ClG 00 33 53.1 -07 52 10           ~ 35 0
5 ACO 68 ClG 00 37 06.2 +09 09 33           ~ 195 0
6 ACO 2813 ClG 00 43 22.8 -20 37 21           ~ 111 0
7 ACO 115 ClG 00 55 59 +26 23.2           ~ 295 1
8 ZwCl 0104+5350 ClG 01 07 43.2 +54 08 43           ~ 35 0
9 ACO 2895 ClG 01 18 07.985 -26 58 00.42           ~ 54 0
10 ACO 209 ClG 01 31 52.9 -13 36 53           ~ 326 0
11 ClG J0142+2131 ClG 01 42 03.1 +21 30 39           ~ 60 1
12 ACO 267 ClG 01 52 43.016 +00 59 58.90           ~ 241 0
13 ACT-CL J0246.4-2033 ClG 02 46 24.9 -20 33 27           ~ 23 0
14 ACO 384 ClG 02 48 08.3 -02 16 37           ~ 35 0
15 ACO 3088 ClG 03 07 02.12 -28 39 57.3           ~ 78 0
16 ACT-CL J0438.9+0716 ClG 04 39 00.7 +07 15 45           ~ 62 0
17 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 465 0
18 ACO 545 ClG 05 32 24.4152 -11 32 35.080           ~ 102 0
19 MCXC J0616.3-2156 ClG 06 16 21.5 -21 56 30           ~ 27 0
20 ZwCl 0634+4750 ClG 06 38 07.5 +47 47 27           ~ 48 0
21 ClG 0657-56 ClG 06 58 26.9 -55 58 21           ~ 1077 1
22 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 275 0
23 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 457 0
24 ACO 3411 ClG 08 41 47.7 -17 28 46           ~ 81 0
25 ACO 746 ClG 09 09 34.7638 +51 32 56.134           ~ 55 0
26 ACO 773 ClG 09 17 51.3 +51 43 20           ~ 308 0
27 ACO 781 ClG 09 20 25.4 +30 30 07           ~ 167 0
28 ACO 1132 ClG 10 58 32.05 +56 47 14.2           ~ 145 1
29 ACO 1351 ClG 11 42 24.7795 +58 32 05.558           ~ 90 0
30 ACO 1423 ClG 11 57 17.3206 +33 36 39.364           ~ 181 0
31 ACO 1443 ClG 12 01 12.1 +23 05 57           ~ 53 0
32 ACO 1451 ClG 12 03 17.3 -21 32 05           ~ 50 0
33 ACO 1576 ClG 12 36 59.5 +63 11 18           ~ 116 0
34 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1178 0
35 BAX 199.3086-25.5133 ClG 13 14 25.4 -25 15 44           ~ 118 0
36 ACO 1733 ClG 13 26 08.78 +02 12 25.7           ~ 8 0
37 ACO 1758 ClG 13 32 32.1 +50 30 37           ~ 266 2
38 ACO 1763 ClG 13 35 20.1 +41 00 04           ~ 335 0
39 ACO 1914 ClG 14 25 57.4 +37 49 54           ~ 338 0
40 ACO 1995 ClG 14 52 55.0 +58 02 59           ~ 140 0
41 ACO 2034 ClG 15 10 03.9 +33 30 57           ~ 248 1
42 2MASX J15150305-1521537 ClG 15 14.9 -15 23           ~ 57 0
43 ACO 2104 ClG 15 40 06.8 -03 17 39           ~ 113 0
44 ACO 2146 ClG 15 56 04.7 +66 20 24           ~ 192 0
45 ACO 2142 ClG 15 58 26.5 +27 13 52           ~ 825 0
46 ACO 2163 ClG 16 15 46.1 -06 08 50           ~ 586 0
47 ACO 2218 ClG 16 35 54.0 +66 13 00           ~ 827 1
48 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 381 0
49 ACO 2255 ClG 17 12 56.0 +64 04 06           ~ 605 0
50 ACO 2261 ClG 17 22 26.9 +32 07 58           ~ 370 0
51 ACO 2345 ClG 21 27 05.391 -12 09 07.41           ~ 151 0
52 NVSS J212709-120958 Rad 21 27 09.27 -12 10 01.5           ~ 132 1
53 ACO 2355 ClG 21 35 18.70 +01 25 27.0           ~ 75 0
54 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 732 2
55 ACO 3888 ClG 22 34 26.3 -37 44 29           ~ 151 1
56 ACO 2537 ClG 23 08 22.3 -02 11 29           ~ 152 0
57 ACO 2631 ClG 23 37 40.7 +00 16 35           ~ 183 0
58 ACO 2645 ClG 23 41 17.0 -09 01 11           ~ 98 0

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