2012A&A...537A.142B


Query : 2012A&A...537A.142B

2012A&A...537A.142B - Astronomy and Astrophysics, volume 537A, 142-142 (2012/1-1)

An XMM-Newton spatially-resolved study of metal abundance evolution in distant galaxy clusters.

BALDI A., ETTORI S., MOLENDI S., BALESTRA I., GASTALDELLO F. and TOZZI P.

Abstract (from CDS):

We present an XMM-Newton analysis of the X-ray spectra of 39 clusters of galaxies at 0.4<z<1.4, covering a temperature range of 1.5≲kT≲11keV. The main goal of this paper is to study how the abundance evolves with redshift not only by means of a single emission measurement performed on the whole cluster but also by spatially resolving the cluster emission. We performed a spatially resolved spectral analysis, using Cash statistics and modeling the XMM-Newton background instead of subtracting it, by analyzing the contribution of the core emission to the observed metallicity. We do not observe a statistically significant (>2σ) abundance evolution with redshift. The most significant deviation from no evolution (at a 90% confidence level) is observed by considering the emission from the whole cluster (r<0.6r500), which can be parametrized as Z∝(1+z)–0.8±0.5. Dividing the emission into three radial bins, no significant evidence of abundance evolution is observed when fitting the data with a power law. We find close agreement with measurements presented in previous studies. Computing the error-weighted mean of the spatially resolved abundances into three redshift bins, we find that it is consistent with being constant with redshift. Although the large error bars in the measurement of the weighted-mean abundance prevent us from claiming any statistically significant spatially resolved evolution, the trend with z in the 0.15-0.4r500 radial bin complements nicely previous measurements and broadly agrees with theoretical predictions. We also find that the data points derived from the spatially resolved analysis are well-fitted by the relation Z(r,z)=Z0(1+(r/0.15r500)2)–a((1+z)/1.6)–γ, where Z0=0.36±0.03, a=0.32±0.07, and γ=0.25±0.57, which represents a significant negative trend of Z with radius and no significant evolution with redshift. We present the first attempt to determine the evolution of abundance at different positions in the clusters and with redshift. However, the sample size and the low-quality data statistics associated with most of the clusters studied prevents us from drawing any statistically significant conclusion about the different evolutionary path that the different regions of the clusters may have traversed.

Abstract Copyright:

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

Simbad objects: 40

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Number of rows : 40
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 BAX 004.5700+16.2958 ClG 00 18 17.0 +16 17 40       19.85   ~ 26 0
2 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 502 0
3 BAX 004.6896+16.0281 ClG 00 18 48.2 +16 02 14           ~ 15 0
4 ClG J0030+2618 ClG 00 30 33.6 +26 18 16           ~ 61 0
5 ClG J0152-1358 ClG 01 52 41.3 -13 58 13           ~ 258 3
6 BAX 035.2850+19.9739 ClG 02 21 08.4 +19 58 26           ~ 11 0
7 RzCS 392 ClG 02 24 04.19 -04 13 26.6           ~ 44 0
8 ClG 0302+17 ClG 03 05 19.0 +17 28 38     21.00     ~ 56 0
9 ClG 0451-03 ClG 04 54 10.9 -03 01 07     20.0     ~ 352 0
10 ClG J0522-3624 ClG 05 22 13.8 -36 24 49           ~ 38 0
11 NAME SEP reg 06 00 00.000 -66 33 38.55           ~ 173 0
12 ClG J0647+7015 ClG 06 47 50.0 +70 14 55           ~ 153 0
13 ClG J0744+3927 ClG 07 44 52.5 +39 27 30           ~ 181 0
14 ClG J0848+4456 ClG 08 48 46.9 +44 56 22           ~ 62 1
15 MCXC J0856.1+3756 ClG 08 56 13.7 +37 56 08           ~ 18 0
16 2MASS J09134545+4056282 Sy2 09 13 45.4951283928 +40 56 28.215343572   19.69 19.21     ~ 250 2
17 ACO 851 ClG 09 43 01.2 +46 59 54   18.9       ~ 327 0
18 ClG J1003+3253 ClG 10 03 04.1 +32 54 28           ~ 29 0
19 ClG 1054-03 ClG 10 57 00.2 -03 37 27     22     ~ 454 0
20 ClG J1103+3555 ClG 11 03 37.1 +35 55 18           ~ 12 0
21 ClG J1120+4318 ClG 11 20 07.6 +43 18 07           ~ 60 0
22 ClG 1137+66 ClG 11 40 23.0 +66 08 16     21.0     ~ 138 0
23 MCS J1206.2-0847 ClG 12 06 12.2 -08 48 02           ~ 246 0
24 ClG J1213+0253 ClG 12 13 34.4 +02 53 57           ~ 30 0
25 ClG J1216-1201 ClG 12 16 45.10 -12 01 17.3           ~ 68 0
26 ClG J1226+3332 ClG 12 26 57.7 +33 32 50           ~ 215 0
27 ClG J1252-2927 ClG 12 52 54.4 -29 27 17           ~ 156 0
28 ClG J1311-0551 ClG 13 11 30.2 -05 51 26           ~ 11 0
29 ZwCl 1332+5043 ClG 13 34 20.0 +50 30 54           ~ 41 0
30 BAX 205.7046+40.4697 ClG 13 42 49.1 +40 28 11           ~ 21 0
31 ClG J1347-1145 ClG 13 47 30.5 -11 45 07           ~ 548 0
32 ClG J1354-0221 ClG 13 54 16.9 -02 21 47           ~ 46 0
33 BAX 214.8479+06.6450 ClG 14 19 23.5 +06 38 42           ~ 13 0
34 WARPS J1419.9+0634E ClG 14 20 00.2 +06 34 53           ~ 5 0
35 ClG J1429+4241 ClG 14 29 06.4 +42 41 10           ~ 26 0
36 ClG 2053-04 ClG 20 56 21.2 -04 37 46   21.0       ~ 165 0
37 ClG J2146+0422 ClG 21 46 04.8 +04 23 19           ~ 23 0
38 BAX 337.1433+20.6131 ClG 22 28 32.6 +20 37 08           ~ 117 0
39 ClG J2235-2557 ClG 22 35 20.6 -25 57 42           ~ 147 0
40 MCXC J2359.5-3211 ClG 23 59 35.7 -32 11 07           ~ 11 0

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