2017A&A...604A.100G


Query : 2017A&A...604A.100G

2017A&A...604A.100G - Astronomy and Astrophysics, volume 604A100-100 (2017/8-1)

On the evolution of the entropy and pressure profiles in X-ray luminous galaxy clusters at z > 0.4.

GHIRARDINI V., ETTORI S., AMODEO S., CAPASSO R. and SERENO M.

Abstract (from CDS):

Context. Galaxy clusters are the most recent products of hierarchical accretion over cosmological scales. The gas accreted from the cosmic field is thermalized inside the cluster halo. Gas entropy and pressure are expected to have a self-similar behaviour with their radial distribution following a power law and a generalized Navarro-Frenk-White profile, respectively. This has also been shown in many different hydrodynamical simulations.
Aims. We derive the spatially resolved thermodynamical properties of 47 X-ray galaxy clusters observed with Chandra in the redshift range 0.4<z<1.2, which is one of the largest samples investigated so far with X-ray spectroscopy and masses reconstructed via the hydrostatic equilibrium equation, with particular care taken to reconstruct the gas entropy and pressure radial profiles. We search for deviation from the self-similar behaviour and look for possible evolution with redshift.
Methods. Under the assumption of a spherically symmetric distribution of the intracluster plasma, we combine the deprojected gas density and deprojected spectral temperature profiles via the hydrostatic equilibrium equation to constrain the concentration and scale radius, which are the parameters that describe a Navarro-Frenk-White profile for each of the clusters in our sample. The temperature profile, which combined with the observed gas density profile reproduces the best-fit mass model, is then used to reconstruct the profiles of entropy and pressure. These profiles cover a median radial interval of [0.04R500-0.76R500]. After interpolating on the same radial grid and partially extrapolating up to R500, these profiles are then stacked in three independent redshift bins to increase the precision of the analysis. The gas mass fraction is then used to improve the self-similar behaviour of the profiles by reducing the scatter among the profiles by a factor 3.
Results. The entropy and pressure profiles lie very close to the baseline prediction from gravitational structure formation. We show that these profiles deviate from the baseline prediction as function of redshift, in particular at z>0.75, where, in the central regions, we observe higher values of the entropy (by a factor of ∼2.2) and systematically lower estimates (by a factor of ∼2.5) of the pressure. The effective polytropic index, which retains information about the thermal distribution of the gas, shows a slight linear positive evolution with the redshift and concentration of the dark matter distribution. A prevalence of non-cool core, disturbed systems, as we observe at higher redshifts, can explain such behaviours.

Abstract Copyright: © ESO, 2017

Journal keyword(s): galaxies: clusters: intracluster medium - galaxies: clusters: general - X-rays: galaxies: clusters - intergalactic medium - intergalactic medium

Simbad objects: 47

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Number of rows : 47
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 ACT-CL J0000.9-5748 ClG 00 01 00 -57 48.5           ~ 57 0
2 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 517 0
3 ACT-CL J0159.8-0849 ClG 01 59 49.4 -08 50 00           ~ 98 0
4 ACT-CL J0257.1-2325 ClG 02 57 09.151 -23 26 05.83           ~ 80 0
5 RX J0329.6-0211 ClG 03 29 41.6 -02 11 47           ~ 155 0
6 ClG 0451-03 ClG 04 54 10.9 -03 01 07     20.0     ~ 368 0
7 ClG J0522-3624 ClG 05 22 13.8 -36 24 49           ~ 41 0
8 ClG J0542-4100 ClG 05 42 49.9 -40 59 58           ~ 67 0
9 ACT-CL J0546.6-5345 ClG 05 46 37.6557 -53 45 33.242           ~ 98 0
10 ClG J0647+7015 ClG 06 47 50.0 +70 14 55           ~ 177 0
11 ClG J0717+3745 ClG 07 17 36.50 +37 45 23.0           ~ 511 0
12 ClG J0744+3927 ClG 07 44 52.5 +39 27 30           ~ 189 0
13 ClG J0848+4453 ClG 08 48 34.800 +44 53 41.90           ~ 124 1
14 ACT-CL J0911.1+1746 ClG 09 11 11.277 +17 46 31.94           ~ 79 0
15 ClG 1054-03 ClG 10 57 00.2 -03 37 27     22     ~ 458 0
16 ClG J1113-2615 ClG 11 13 05.7 -26 15 36           ~ 37 0
17 ClG J1117+1744 ClG 11 17 30.2 +17 44 44           ~ 35 0
18 ClG J1120+4318 ClG 11 20 07.6 +43 18 07           ~ 65 0
19 ClG 1137+66 ClG 11 40 23.0 +66 08 16     21.0     ~ 141 0
20 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 546 0
21 MCS J1206.2-0847 ClG 12 06 12.2 -08 48 02           ~ 286 0
22 ClG J1221+4918 ClG 12 21 25.0 +49 18 07           ~ 60 0
23 ClG J1226+3332 ClG 12 26 57.7 +33 32 50           ~ 228 0
24 XMMXCS J123017.1+133903.8 ClG 12 30 17.100 +13 39 03.80           ~ 4 0
25 ClG J1252-2927 ClG 12 52 54.4 -29 27 17           ~ 158 0
26 ClG J1311-0311 ClG 13 11 01.7 -03 10 38           ~ 120 0
27 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 577 0
28 ClG J1350+6007 ClG 13 50 48.55 +60 07 06.7           ~ 46 0
29 ClG J1415+3611 ClG 14 15 11.1 +36 12 03           ~ 85 1
30 LCDCS 0954 ClG 14 20 29.7 -11 34 04           ~ 7 0
31 ClG J1423+2404 ClG 14 23 47.7 +24 04 40           ~ 231 0
32 ClG J1524+0957 ClG 15 24 40.3 +09 57 35           ~ 64 0
33 ClG J1621+3810 ClG 16 21 25.5 +38 09 43           ~ 83 0
34 ClG 1621+26 ClG 16 23 35.7 +26 33 50           ~ 145 0
35 ClG J1701+6414 ClG 17 01 22.6 +64 14 09           ~ 78 0
36 ClG J1716+6708 ClG 17 16 49.6 +67 08 30           ~ 137 0
37 ACT-CL J2043.2-5035 ClG 20 43 16.7205 -50 35 30.861           ~ 47 0
38 ClG 2053-04 ClG 20 56 21.2 -04 37 46   21.0       ~ 168 0
39 ACT-CL J2106.0-5844 ClG 21 06 04.3 -58 44 32           ~ 103 0
40 ClG J2129-0741 ClG 21 29 26.0 -07 41 28           ~ 189 0
41 ACT-CL J2214.9-1359 ClG 22 14 57.3 -14 00 12           ~ 100 0
42 BAX 337.1433+20.6131 ClG 22 28 32.6 +20 37 08           ~ 132 0
43 ClG J2243-0935 ClG 22 43 21.1 -09 35 43           ~ 96 0
44 ClG J2302+0844 ClG 23 02 48.1 +08 43 50           ~ 43 0
45 CDGS 50 ClG 23 18 30.670 +00 34 03.03           ~ 19 0
46 ACT-CL J2327.4-0204 ClG 23 27 27.60 -02 04 37.4           ~ 44 0
47 ACT-CL J2337.4-5942 ClG 23 37 24.2 -59 42 17           ~ 52 0

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