2019A&A...628A..86B


Query : 2019A&A...628A..86B

2019A&A...628A..86B - Astronomy and Astrophysics, volume 628A, 86-86 (2019/8-1)

The Most Massive galaxy Clusters (M2C) across cosmic time: link between radial total mass distribution and dynamical state.

BARTALUCCI I., ARNAUD M., PRATT G.W., DEMOCLES J. and LOVISARI L.

Abstract (from CDS):

We study the dynamical state and the integrated total mass profiles of 75 massive (M500>5x1014M) Sunyaev-Zeldovich(SZ)-selected clusters at 0.08<z<1.1. The sample is built from the Planck catalogue, with the addition of four SPT clusters at z>0.9. Using XMM-Newton imaging observations, we characterise the dynamical state with the centroid shift <w>, the concentration CSB, and their combination, M, which simultaneously probes the core and the large-scale gas morphology. Using spatially resolved spectroscopy and assuming hydrostatic equilibrium, we derive the total integrated mass profiles. The mass profile shape is quantified by the sparsity, that is the ratio of M500 to M2500, the masses at density contrasts of 500 and 2500, respectively. We study the correlations between the various parameters and their dependence on redshift. We confirm that SZ-selected samples, thought to most accurately reflect the underlying cluster population, are dominated by disturbed and non-cool core objects at all redshifts. There is no significant evolution or mass dependence of either the cool core fraction or the centroid shift parameter. The M parameter evolves slightly with z, having a correlation coefficient of ρ=-0.2±0.1 and a null hypothesis p-value of 0.01. In the high-mass regime considered here, the sparsity evolves minimally with redshift, increasing by 10% between z<0.2 and z>0.55, an effect that is significant at less than 2σ. In contrast, the dependence of the sparsity on dynamical state is much stronger, increasing by a factor of ∼60% from the one third most relaxed to the one third most disturbed objects, an effect that is significant at more than 3σ. This is the first observational evidence that the shape of the integrated total mass profile in massive clusters is principally governed by the dynamical state and is only mildly dependent on redshift. We discuss the consequences for the comparison between observations and theoretical predictions.

Abstract Copyright: © I. Bartalucci et al. 2019

Journal keyword(s): dark matter - galaxies: clusters: intracluster medium - X-rays: galaxies: clusters

Simbad objects: 75

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Number of rows : 75
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 2744 ClG 00 14 20.03 -30 23 17.8           ~ 812 0
2 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 502 0
3 ACO 2813 ClG 00 43 32.377 -20 35 23.51           ~ 96 0
4 ACT-CL J0049.1-2440 ClG 00 49 10.9 -24 40 43           ~ 14 0
5 ACT-CL J0137.4-0827 ClG 01 37 24.9 -08 27 22           ~ 34 0
6 ACT-CL J0200.2-2454 ClG 02 00 16.3 -24 54 52           ~ 13 0
7 ACT-CL J0232.2-4421 ClG 02 32 18.69 -44 20 41.5           ~ 110 0
8 ACT-CL J0243.5-4833 ClG 02 43 38.873 -48 33 38.94           ~ 20 0
9 PLCKESZ G147.3-16.6 ClG 02 56 +40.3           ~ 9 0
10 MCXC J0303.7-7752 ClG 03 03 48.4 -77 52 41           ~ 28 0
11 PSZ1 G193.29-46.13 ClG 03 35 51.40 -06 58 32.8           ~ 9 0
12 PSZ1 G254.59-45.23 ClG 04 17 33.9474 -47 47 55.745           ~ 27 0
13 ACT-CL J0446.7-3703 ClG 04 46 47.7 -37 03 50           ~ 11 0
14 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 436 0
15 ClG 0451-03 ClG 04 54 10.9 -03 01 07     20.0     ~ 352 0
16 ACT-CL J0454.7-2016 ClG 04 54 45.4 -20 17 07           ~ 10 0
17 ACT-CL J0528.8-3927 ClG 05 28 56.2 -39 27 49           ~ 68 0
18 ACT-CL J0532.9-3701 ClG 05 32 56.4 -37 01 34           ~ 48 0
19 ACT-CL J0546-5346 ClG 05 46 35.0 -53 46 04           ~ 86 0
20 ACO 3364 ClG 05 47 38.1 -31 52 15           ~ 75 0
21 ACO 3378 ClG 06 05 53.7 -35 18 06           ~ 81 1
22 PLCKESZ G266.6-27.3 ClG 06 15 56.2665 -57 45 50.508           ~ 59 0
23 ACT-CL J0616.5-5227 ClG 06 16 34.20 -52 27 13.3           ~ 25 0
24 ACO 3404 ClG 06 45 29.50 -54 13 37.0           ~ 96 0
25 ClG J0647+7015 ClG 06 47 50.0 +70 14 55           ~ 153 0
26 ClG 0657-56 ClG 06 58 29.6 -55 56 39           ~ 963 1
27 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 463 0
28 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 437 0
29 PSZ1 G183.92+42.99 ClG 09 10 51.0 +38 50 22           ~ 21 0
30 ACT-CL J0911.1+1746 ClG 09 11 11.277 +17 46 31.94           ~ 72 0
31 ACO 773 ClG 09 17 51.3 +51 43 20           ~ 295 0
32 ACO 781 ClG 09 20 25.4 +30 30 07           ~ 153 0
33 ACO 868 ClG 09 45 28.1 -08 38 51           ~ 60 0
34 ACO 963 ClG 10 17 03.4 +39 02 56           ~ 400 0
35 PSZ1 G212.51+63.18 ClG 10 52 52.4 +24 15 30           ~ 14 0
36 ACO 1300 ClG 11 32 00.7 -19 53 34           ~ 151 0
37 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 460 0
38 ACO 1413 ClG 11 55 12.87 +23 23 46.9           ~ 430 0
39 MCS J1206.2-0847 ClG 12 06 12.2 -08 48 02           ~ 246 0
40 ACO 1576 ClG 12 36 59.5 +63 11 18           ~ 108 0
41 ACO 1650 ClG 12 58 42.0 -01 45 45           ~ 304 0
42 ACO 1651 ClG 12 59 22.43 -04 11 47.1           ~ 290 0
43 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1125 0
44 ACO 1763 ClG 13 35 20.1 +41 00 04           ~ 312 0
45 PSZ1 G099.84+58.45 ClG 14 14 48.09 +54 46 42.2           ~ 27 0
46 ClG J1420+3955 ClG 14 20 40.38 +39 55 10.6           ~ 27 0
47 ACO 1914 ClG 14 26 03.32 +37 49 58.7           ~ 314 0
48 eMACS J1508.1+5755 ClG 15 08 21.9 +57 55 15           ~ 23 0
49 ACO 2034 ClG 15 10 12.96 +33 29 53.2           ~ 215 1
50 PSZ1 G045.85+57.71 ClG 15 18 20.6 +29 27 36           ~ 23 0
51 PSZ1 G070.91+49.26 ClG 15 56 42.9816 +44 39 11.750           ~ 15 0
52 ACO 2163 ClG 16 15 46.1 -06 08 50           ~ 562 0
53 ACO 2204 ClG 16 32 45.7 +05 34 43           ~ 436 0
54 ACO 2218 ClG 16 35 54.0 +66 13 00           ~ 809 1
55 ACO 2219 ClG 16 40 22.1 +46 42 20           ~ 359 0
56 ACO 2255 ClG 17 12 50.04 +64 03 10.6           ~ 568 0
57 PSZ1 G046.13+30.75 ClG 17 17 05.8 +24 04 26           ~ 13 0
58 ClG J1720+2638 ClG 17 20 09.6 +26 37 35           ~ 255 0
59 PLCKESZ G004.5-19.5 ClG 19 16 54 -33 30.5           ~ 26 0
60 ACT-CL J1920.9-4550 ClG 19 20 59.8 -45 51 00           ~ 8 0
61 ACT-CL J2106.0-5844 ClG 21 06 04.3 -58 44 32           ~ 90 0
62 ClG J2129-0741 ClG 21 29 26.0 -07 41 28           ~ 172 0
63 ACT-CL J2146.5-4633 ClG 21 46 34.8 -46 32 56           ~ 28 0
64 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 688 2
65 ACO 3827 ClG 22 01 49.1 -59 57 15           ~ 159 0
66 ACT-CL J2214.9-1359 ClG 22 14 57.3 -14 00 12           ~ 88 0
67 ACO 3854 ClG 22 17 45.72 -35 43 31.4           ~ 67 0
68 ACO 3856 ClG 22 18 45.2 -38 53 57           ~ 79 2
69 BAX 337.1433+20.6131 ClG 22 28 32.6 +20 37 08           ~ 117 0
70 ACO 3888 ClG 22 34 23.0 -37 43 29           ~ 138 1
71 ClG J2243-0935 ClG 22 43 21.1 -09 35 43           ~ 78 0
72 ACO 3911 ClG 22 46 22.6 -52 44 21           ~ 64 0
73 ACO S 1063 ClG 22 48 45.4 -44 31 42           ~ 320 0
74 ACO 3921 ClG 22 49 59.0 -64 25 48           ~ 150 1
75 ACT-CL J2341.2-5119 ClG 23 41 12.3 -51 19 43           ~ 44 0

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