2014A&A...567A..83K


Query : 2014A&A...567A..83K

2014A&A...567A..83K - Astronomy and Astrophysics, volume 567A83-83 (2014/7-1)

X-ray AGN in the XMM-LSS galaxy clusters: no evidence of AGN suppression.

KOULOURIDIS E., PLIONIS M., MELNYK O., ELYIV A., GEORGANTOPOULOS I., CLERC N., SURDEJ J., CHIAPPETTI L. and PIERRE M.

Abstract (from CDS):

We present a study of the overdensity of X-ray-selected active galactic nuclei (AGN) in 33 galaxy clusters in the XMM-LSS field (The XMM-Newton Large Scale Structure Survey), up to redshift z=1.05 and further divided into a lower (0.14≤z≤0.35) and a higher redshift (0.43≤z≤1.05) subsample. Previous studies have shown that the presence of X-ray-selected AGN in rich galaxy clusters is suppressed, since their number is significantly lower than what is expected from the high galaxy overdensities in the area. In the current study we have investigated the occurrence of X-ray-selected AGN in low (<Lx,bol≥2.7x1043erg/s) and moderate (<Lx,bol≥2.4x1044erg/s) X-ray luminosity galaxy clusters in an attempt to trace back the relation between high-density environments and nuclear activity. Owing to the wide contiguous XMM-LSS survey area, we were able to extend the study to the cluster outskirts. We therefore determined the projected overdensity of X-ray point-like sources around each cluster out to 6r500 radius, within δr500=1 annulus, with respect to the field expectations based on the X-ray source logN-logS of the XMM-LSS field. To provide robust statistical results we also conducted a consistent stacking analysis separately for the two z ranges. We investigated whether the observed X-ray overdensities are to be expected thanks to the obvious enhancement of galaxy numbers in the cluster environment by also estimating the corresponding optical galaxy overdensities, and we assessed the possible enhancement or suppression of AGN activity in clusters. We find a positive X-ray projected overdensity in both redshift ranges at the first radial bins, which however has the same amplitude as that of optical galaxies. Therefore, no suppression (or enhancement) of X-ray AGN activity with respect to the field is found, in sharp contrast to previous results based on rich galaxy clusters, implying that the mechanisms responsible for the suppression are not as effective in lower density environments. After a drop to roughly the background level between 2 and 3r500, the X-ray overdensity exhibits a rise at larger radii, significantly greater than the corresponding optical overdensity. The radial distance of this overdensity ``bump'', corresponding to ∼1.5-3Mpc, depends on the richness of the clusters, as well as on the overall X-ray overdensity profile. Finally, using the redshift information, photometric or spectroscopic, of the optical counterparts, we derive the spatial overdensity profile of the clusters. We find that the agreement between X-ray and optical overdensities in the first radial bins is also suggested in the 3-dimensional analysis. However, we argue that the X-ray overdensity ``bump'' at larger radial distance is at least partially a result of flux boosting by gravitational lensing of background quasi-stellar objects, confirming previous results. For high-redshift clusters, the enhancement of X-ray AGN activity in their outskirts appears to be intrinsic. We argue that a spatial analysis is crucial for disentangling irrelevant phenomena affecting the projected analysis, but we are still not able to report statistically significant results on the spatial overdensity of AGN in clusters or their outskirts because we lack the necessary numbers.

Abstract Copyright: ∼

Journal keyword(s): galaxies: clusters: general - galaxies: active - X-rays: galaxies: clusters - galaxies: interactions - galaxies: evolution - large-scale structure of Universe

Simbad objects: 34

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Number of rows : 34
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 HSCS J021444-034921 ClG 02 14 43.71 -03 49 21.4           ~ 9 0
2 ACT-CL J0215.3-0343 ClG 02 15 23.99 -03 43 32.2           ~ 41 0
3 ACT-CL J0215.4-0440 ClG 02 15 29 -04 40.9           ~ 25 0
4 HSCS J021548-045015 ClG 02 15 48 -04 50.5           ~ 10 0
5 ACO 334 ClG 02 16 12.2 -04 14 31           ~ 21 0
6 HSCS J021735-051330 ClG 02 17 34.49 -05 13 18.5           ~ 22 0
7 NAME XMM-LSS Field reg 02 18 00 -07 00.0           ~ 347 0
8 HSCS J021805-033923 ClG 02 18 05 -03 39.4           ~ 8 0
9 HSCS J021824-052501 ClG 02 18 25.11 -05 24 51.7           ~ 10 0
10 XCLASS 1706 ClG 02 19 44.31 -04 53 15.4           ~ 13 0
11 RzCS 024 ClG 02 20 23.5 -02 50 27           ~ 8 0
12 RzCS 031 ClG 02 20 45.46 -03 25 59.7           ~ 26 0
13 ACT-CL J0221.7-0346 ClG 02 21 45.8 -03 46 08           ~ 55 0
14 HSCS J022156-054532 ClG 02 21 56 -05 45.4           ~ 23 0
15 XCLASS 169 ClG 02 22 05.6 -04 32 47           ~ 25 0
16 HSCS J022207-030314 ClG 02 22 06.85 -03 03 14.5           ~ 20 0
17 HSCS J022253-032823 ClG 02 22 53.6 -03 28 28           ~ 17 0
18 RzCS 105 ClG 02 23 56.300 -03 05 59.30           ~ 15 0
19 HSCS J022358-043505 ClG 02 23 57.4 -04 35 17           ~ 25 0
20 HSCS J022402-050527 ClG 02 24 00.6 -05 05 25           ~ 29 0
21 RzCS 447 ClG 02 24 27.0 -04 50 34           ~ 13 0
22 CXOU J022428.2-041529 ClG 02 24 33.8 -04 14 15           ~ 36 0
23 HSCS J022457-034853 ClG 02 24 57.1 -03 48 53           ~ 30 0
24 RzCS 774 ClG 02 25 20.2 -03 48 30           ~ 18 0
25 HSCS J022525-044045 ClG 02 25 24.6 -04 40 45       17.3   ~ 43 0
26 XMDS 243 ClG 02 25 31 -04 14.3           ~ 39 0
27 HSCS J022532-035509 ClG 02 25 32.48 -03 55 09.5           ~ 20 0
28 MARD J022536.2-030928 ClG 02 25 40.6 -03 11 21           ~ 22 0
29 XCLASS 39 ClG 02 25 59.5 -02 49 35           ~ 12 0
30 RzCS 119 ClG 02 27 09.7 -04 18 05           ~ 32 1
31 RzCS 768 ClG 02 27 22.39 -03 21 39.2           ~ 30 0
32 HSCS J022725-043237 ClG 02 27 25.9 -04 32 15           ~ 35 0
33 ACT-CL J0227.6-0317 ClG 02 27 38.20 -03 17 56.9           ~ 32 0
34 RzCS 180 ClG 02 27 40.3 -04 51 31           ~ 33 0

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