2013ApJ...777..141C


Query : 2013ApJ...777..141C

2013ApJ...777..141C - Astrophys. J., 777, 141 (2013/November-2)

Revisiting scaling relations for giant radio halos in galaxy clusters.

CASSANO R., ETTORI S., BRUNETTI G., GIACINTUCCI S., PRATT G.W., VENTURI T., KALE R., DOLAG K. and MARKEVITCH M.

Abstract (from CDS):

Many galaxy clusters host megaparsec-scale radio halos, generated by ultrarelativistic electrons in the magnetized intracluster medium. Correlations between the synchrotron power of radio halos and the thermal properties of the hosting clusters were established in the last decade, including the connection between the presence of a halo and cluster mergers. The X-ray luminosity and redshift-limited Extended GMRT Radio Halo Survey provides a rich and unique dataset for statistical studies of the halos. We uniformly analyze the radio and X-ray data for the GMRT cluster sample, and use the new Planck Sunyaev-Zel'dovich (SZ) catalog to revisit the correlations between the power of radio halos and the thermal properties of galaxy clusters. We find that the radio power at 1.4 GHz scales with the cluster X-ray (0.1-2.4 keV) luminosity computed within R500 as P1.4 ∼ L5002.1±0.2. Our bigger and more homogenous sample confirms that the X-ray luminous (L500> 5x1044 erg/s) clusters branch into two populations–radio halos lie on the correlation, while clusters without radio halos have their radio upper limits well below that correlation. This bimodality remains if we excise cool cores from the X-ray luminosities. We also find that P1.4 scales with the cluster integrated SZ signal within R500, measured by Planck, as P1.4 ∼ Y5002.05±0.28, in line with previous findings. However, contrary to previous studies that were limited by incompleteness and small sample size, we find that "SZ-luminous" Y500> 6x10–5 Mpc2 clusters show a bimodal behavior for the presence of radio halos, similar to that in the radio-X-ray diagram. Bimodality of both correlations can be traced to clusters dynamics, with radio halos found exclusively in merging clusters. These results confirm the key role of mergers for the origin of giant radio halos, suggesting that they trigger the relativistic particle acceleration.

Abstract Copyright:

Journal keyword(s): galaxies: clusters: general - radiation mechanisms: non-thermal - radio continuum: general - X-rays: galaxies: clusters

Simbad objects: 57

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Number of rows : 57
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 2697 ClG 00 03 11.5 -06 05 30           ~ 47 0
2 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 813 0
3 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 502 0
4 BAX 006.9575+26.2739 ClG 00 27 45.90 +26 16 25.0           ~ 39 0
5 ACO 141 ClG 01 05 37.183 -24 40 49.95           ~ 79 0
6 ZwCl 0104+0048 ClG 01 06 50.5 +01 04 10           ~ 61 0
7 ACO 209 ClG 01 31 52.9 -13 36 53           ~ 295 0
8 ClG J0142+2131 ClG 01 42 03.1 +21 30 39           ~ 56 1
9 ACO 267 ClG 01 52 43.016 +00 59 58.90           ~ 230 0
10 ACO 3088 ClG 03 07 02.12 -28 39 57.3           ~ 70 0
11 PLCKESZ G171.9-40.7 ClG 03 12 55 +08 22.8           ~ 48 0
12 ACT-CL J0437.1+0043 ClG 04 37 12.0820 +00 43 37.737           ~ 43 0
13 ACT-CL J0438.9+0716 ClG 04 39 00.7 +07 15 45           ~ 58 0
14 BAX 069.7593+05.3453 ClG 04 39 02.2 +05 20 43           ~ 78 0
15 ACO 521 ClG 04 54 08.6 -10 14 39           ~ 249 0
16 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 436 0
17 ACO 545 ClG 05 32 24.4152 -11 32 35.080           ~ 97 0
18 ClG 0657-56 ClG 06 58 29.6 -55 56 39           ~ 963 1
19 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 463 0
20 B3 0714+378 Rad 07 17 36.6 +37 45 01           ~ 170 2
21 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 258 0
22 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 437 0
23 ACO 697 ClG 08 42 57.6 +36 21 45           ~ 253 0
24 ZwCl 0857+2107 ClG 09 00 36.90 +20 53 40.3           ~ 93 0
25 ACO 754 ClG 09 09 08.4 -09 39 58           ~ 666 1
26 ACO 773 ClG 09 17 51.3 +51 43 20           ~ 295 0
27 ACO 781 ClG 09 20 25.4 +30 30 07           ~ 153 0
28 ZwCl 0949+5207 ClG 09 52 49.1 +51 53 05           ~ 135 0
29 ZwCl 1113+0144 ClG 11 15 54.0 +01 29 44           ~ 37 0
30 ACO 1300 ClG 11 32 00.7 -19 53 34           ~ 151 0
31 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 460 0
32 ACO 1423 ClG 11 57 17.3206 +33 36 39.364           ~ 168 0
33 ACO 1576 ClG 12 36 59.5 +63 11 18           ~ 108 0
34 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 4803 2
35 ZwCl 1303+2647 ClG 13 05 58.0 +26 30 53   20.1       ~ 25 0
36 ZwCl 1309+2216 ClG 13 11.5 +22 00           ~ 23 0
37 ACO 1758 ClG 13 32 32.1 +50 30 37           ~ 251 2
38 ACO 1914 ClG 14 26 03.32 +37 49 58.7           ~ 314 0
39 ACO 1995 ClG 14 52 55.0 +58 02 59           ~ 130 0
40 ACO S 780 ClG 14 59 29.1 -18 10 45           ~ 82 0
41 2MASX J15150305-1521537 ClG 15 14.9 -15 23           ~ 46 0
42 LEDA 1900245 Bla 15 32 53.780 +30 20 59.41   19.1   15.7 17.819 ~ 145 0
43 ClG J1532+3021 ClG 15 32 53.8 +30 21 00           ~ 113 0
44 ACO 2146 ClG 15 56 04.7 +66 20 24           ~ 176 0
45 ACO 2163 ClG 16 15 46.1 -06 08 50           ~ 563 0
46 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 359 0
47 ACO 2256 ClG 17 03 09.4 +78 39 36           ~ 885 1
48 ACO 2255 ClG 17 12 50.04 +64 03 10.6           ~ 568 0
49 ACO 2261 ClG 17 22 26.9 +32 07 58           ~ 342 0
50 ACO 2319 ClG 19 20 45.3 +43 57 43           ~ 461 1
51 ACT-CL J2003.5-2323 ClG 20 03 32.3 -23 23 30           ~ 59 0
52 BAX 337.1433+20.6131 ClG 22 28 32.6 +20 37 08           ~ 117 0
53 ACO 2485 ClG 22 48 33 -16 07.1           ~ 49 0
54 ACO 2537 ClG 23 08 22.3 -02 11 29           ~ 137 0
55 ACO 2631 ClG 23 37 40.7 +00 16 35           ~ 171 0
56 ACO 2645 ClG 23 41 17.0 -09 01 11           ~ 90 0
57 ACO 2667 ClG 23 51 39.37 -26 05 02.7           ~ 175 0

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