The XMM-NEWTON Ω project -: I.: The X-ray luminosity-temperature relation at z > 0.4

被引:55
作者
Lumb, DH [1 ]
Bartlett, JG
Romer, AK
Blanchard, A
Burke, DJ
Collins, CA
Nichol, RC
Giard, M
Marty, PB
Nevalainen, J
Sadat, R
Vauclair, SC
机构
[1] European Space Agcy, ESTEC, Sci Payloads & Adv Concepts Off, NL-2200 AG Noordwijk, Netherlands
[2] Univ Paris 07, APC, PCC Coll France, F-75231 Paris 05, France
[3] Ctr Donnees Astronom Strasbourg, F-67000 Strasbourg, France
[4] Carnegie Mellon Univ, Dept Phys, Pittsburgh, PA 15213 USA
[5] Observ Midi Pyrenees, Astrophys Lab, CNRS, UPS, F-31400 Toulouse, France
[6] Harvard Smithsonian Ctr Astrophys, Cambridge, MA 02138 USA
[7] Liverpool John Moores Univ, Astrophys Res Inst, Birkenhead CH41 1LD, Merseyside, England
[8] Ctr Etud Spatiale Rayonnements, F-31028 Toulouse, France
[9] Univ Sussex, Ctr Astron, Dept Phys & Astron, Brighton BN1 9QH, E Sussex, England
关键词
X-rays; galaxies; clusters;
D O I
10.1051/0004-6361:20035687
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We describe XMM-Newton Guaranteed Time observations of a sample of eight high redshift (0.45 < z < 0.62) clusters. The goal of these observations was to measure the luminosity and the temperature of the clusters to a precision of similar to10%, leading to constraints on the possible evolution of the luminosity-temperature (L-x - T-x) relation, and ultimately on the values of the matter density, Omega(M), and, to a lesser extent, the cosmological constant Omega(Lambda). The clusters were drawn from the SHARC and 160 Square Degree (160SD) ROSAT surveys and span a bolometric (0.0-20 keV) luminosity range of 2.0 to 14.4 x 10(44) erg s(-1) (H-0 = 50, Omega(M) = 1, Omega(Lambda) = 0). Here we describe our data analysis techniques and present, for the first time with XMM-Newton, a L, - T, relation. For each of the eight clusters in the sample, we have measured total (r < r(viral)) bolometric luminosities, performed beta-model fits to the radial surface profiles and made spectral fits to a single temperature isothermal model. We describe data analysis techniques that pay particular attention to background mitigation. We have also estimated temperatures and luminosities for two known clusters (Abell 2246 and RX J1325.0-3814), and one new high redshift cluster candidate (XMMU J084701.8+345117), that were detected off-axis. Characterizing the L-x - T-x relation as L-x = L-6(T/6 keV)(alpha), we find L-6 = 15.9(-5.2)(+7.6) x 10(44) erg s(-1) and alpha = 2.7 +/- 0.4 for an Omega(Lambda) = 0.0,Omega(M) = 1.0, H-0 = 50 km s(-1) Mpc(-1) cosmology at a typical redshift z similar to 0.55. Comparing with the low redshift study by Markevitch (1998), we find a to be in agreement, and assuming L-x - T-x to evolve as (1 + z)(A), we find A = 0.68 +/- 0.26 for the same cosmology and A = 1.52(-0.27)(+0.26) for an Omega(Lambda) - 0.7, Omega(M) = 0.3 cosmology. Our A values are very similar to those found previously by Vikhlinin et al. (2002) using a compilation of Chandra observations of 0.39 < z < 1.26 clusters. We conclude that there is now evidence from both XMM-Newton and Chandra for an evolutionary trend in the L, - T, relation. This evolution is significantly below the level expected from the predictions of the self-similar model for an Omega(Lambda) = 0.0,Omega(M) = 1 -0, Cosmology, but consistent with self-similar model in an Omega(Lambda) = 0.7, Omega(M) = 0.3 cosmology. Our observations lend support to the robustness and completeness of the SHARC and 160SD surveys.
引用
收藏
页码:853 / 872
页数:20
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