2007MNRAS.382.1289P


Query : 2007MNRAS.382.1289P

2007MNRAS.382.1289P - Mon. Not. R. Astron. Soc., 382, 1289-1308 (2007/December-2)

The XMM-LSS survey: the Class 1 cluster sample over the initial 5 deg2 and its cosmological modelling.

PACAUD F., PIERRE M., ADAMI C., ALTIERI B., ANDREON S., CHIAPPETTI L., DETAL A., DUC P.-A., GALAZ G., GUEGUEN A., LE FEVRE J.-P., HERTLING G., LIBBRECHT C., MELIN J.-B., PONMAN T.J., QUINTANA H., REFREGIER A., SPRIMONT P.-G., SURDEJ J., VALTCHANOV I., WILLIS J.P., ALLOIN D., BIRKINSHAW M., BREMER M.N., GARCET O., JEAN C., JONES L.R., LE FEVRE O., MACCAGNI D., MAZURE A., PROUST D., ROTTGERING H.J.A. and TRINCHIERI G.

Abstract (from CDS):

We present a sample of 29 galaxy clusters from the XMM-LSS survey over an area of some 5 deg2 out to a redshift of z = 1.05. The sample clusters, which represent about half of the X-ray clusters identified in the region, follow well-defined X-ray selection criteria and are all spectroscopically confirmed. For all clusters, we provide X-ray luminosities and temperatures as well as masses, obtained from dedicated spatial and spectral fitting. The cluster distribution peaks around z = 0.3 and T = 1.5 keV, half of the objects being groups with a temperature below 2 keV. Our LX-T(z) relation points towards self-similar evolution, but does not exclude other physically plausible models. Assuming that cluster scaling laws follow self-similar evolution, our number density estimates up to z = 1 are compatible with the predictions of the concordance cosmology and with the findings of previous ROSAT surveys. Our well-monitored selection function allowed us to demonstrate that the inclusion of selection effects is essential for the correct determination of the evolution of the LX-T relation, which may explain the contradictory results from previous studies. Extensive simulations show that extending the survey area to 10 deg2 has the potential to exclude the non-evolution hypothesis, but those constraints on more refined intracluster medium models will probably be limited by the large intrinsic dispersion of the LX-T relation, whatever be the sample size. We further demonstrate that increasing the dispersion in the scaling laws increases the number of detectable clusters, hence generating further degeneracy [in addition to σ8,Ωm, LX-T(z)] in the cosmological interpretation of the cluster number counts. We provide useful empirical formulae for the cluster mass-flux and mass-count rate relations as well as a comparison between the XMM-LSS mass sensitivity and that of forthcoming Sunyaev-Zel'dovich surveys.

Abstract Copyright: 2007 The Authors. Journal compilation © 2007 RAS

Journal keyword(s): surveys - cosmological parameters - large-scale structure of Universe - X-rays: galaxies: clusters

Simbad objects: 37

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Number of rows : 37
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 NAME XMM-LSS Field reg 02 18 00 -07 00.0           ~ 347 0
2 RzCS 024 ClG 02 20 23.5 -02 50 27           ~ 8 0
3 RzCS 031 ClG 02 20 45.46 -03 25 59.7           ~ 26 0
4 ACT-CL J0221.7-0346 ClG 02 21 45.8 -03 46 08           ~ 55 0
5 XCLASS 169 ClG 02 22 05.6 -04 32 47           ~ 25 0
6 HSCS J022207-030314 ClG 02 22 06.85 -03 03 14.5           ~ 20 0
7 RzCS 065 ClG 02 22 10.7 -02 40 48           ~ 7 0
8 2MASX J02225051-0311544 G 02 22 50.51787 -03 11 54.4450           ~ 1 0
9 HSCS J022253-032823 ClG 02 22 53.6 -03 28 28           ~ 17 0
10 HSCS J022349-025126 ClG 02 23 48.1 -02 51 31           ~ 12 0
11 RzCS 105 ClG 02 23 56.300 -03 05 59.30           ~ 15 0
12 HSCS J022358-043505 ClG 02 23 57.4 -04 35 17           ~ 25 0
13 HSCS J022402-050527 ClG 02 24 00.6 -05 05 25           ~ 29 0
14 RzCS 392 ClG 02 24 04.19 -04 13 26.6           ~ 47 0
15 LEDA 1055937 Sy1 02 24 29.9948667240 -04 36 13.655472120   16.04   15.07   ~ 15 0
16 CXOU J022428.2-041529 ClG 02 24 33.8 -04 14 15           ~ 36 0
17 XCLASS 198 ClG 02 24 56.0 -05 08 02           ~ 18 0
18 6dFGS gJ022456.2-050759 AGN 02 24 56.1507668280 -05 07 59.483806752   16.91   15.48   ~ 22 0
19 HSCS J022457-034853 ClG 02 24 57.1 -03 48 53           ~ 30 0
20 RzCS 774 ClG 02 25 20.2 -03 48 30           ~ 18 0
21 HSCS J022525-044045 ClG 02 25 24.6 -04 40 45       17.3   ~ 43 0
22 LEDA 3092693 G 02 25 29.7848033520 -04 00 41.922086364   15.65   14.24   ~ 17 0
23 XMDS 243 ClG 02 25 31 -04 14.3           ~ 39 0
24 HSCS J022532-035509 ClG 02 25 32.48 -03 55 09.5           ~ 20 0
25 MARD J022536.2-030928 ClG 02 25 40.6 -03 11 21           ~ 22 0
26 XCLASS 39 ClG 02 25 59.5 -02 49 35           ~ 12 0
27 NPM1G -05.0105 EmG 02 26 09.6701490432 -04 58 05.640470580   16.11   14.75   ~ 28 0
28 XLSSC 011 ClG 02 26 10.60 -04 58 11.5           ~ 31 0
29 XCLASS 38 ClG 02 26 16.3 -02 39 57           ~ 14 0
30 NVSS J022617-050443 rG 02 26 17.4459180168 -05 04 43.498080012   16.13   14.82   ~ 25 1
31 MCG-01-07-011 BiC 02 26 58.9925756496 -04 35 27.084907032   16       ~ 15 0
32 RzCS 119 ClG 02 27 09.7 -04 18 05           ~ 32 1
33 RzCS 768 ClG 02 27 22.39 -03 21 39.2           ~ 30 0
34 HSCS J022725-043237 ClG 02 27 25.9 -04 32 15           ~ 35 0
35 ACT-CL J0227.6-0317 ClG 02 27 38.20 -03 17 56.9           ~ 32 0
36 RzCS 180 ClG 02 27 40.3 -04 51 31           ~ 33 0
37 RzCS 185 ClG 02 28 03.4 -04 51 03           ~ 29 0

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