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Stellar and total baryon mass fractions in groups and clusters since redshift 1by: S. Giodini, D. Pierini, A. Finoguenov, G. W. Pratt, H. Boehringer, A. Leauthaud, L. Guzzo, H. Aussel, M. Bolzonella, P. Capak, M. Elvis, G. Hasinger, O. Ilbert, Kartaltepe, A. M. Koekemoer, S. J. Lilly, H. J. Mccracken, M. Salvato, D. B. Sanders, N. Z. Scoville, S. Sasaki, V. Smolcic, Y. Taniguchi, D. Thompson, Cosmos Collaboration
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AbstractWe investigate if the discrepancy between estimates of the total baryon mass fraction obtained from observations of the cosmic microwave background (CMB) and of galaxy groups/clusters persists when a large sample of groups is considered. To this purpose, 91 candidate X-ray groups/poor clusters at redshift 0.1<z<1 are selected from the COSMOS 2 deg^2 survey, based only on their X-ray luminosity and extent. This sample is complemented by 27 nearby clusters for which robust analogous determinations of the total and stellar mass inside R_500 are available. The total sample of 118 groups and clusters with z<1 spans a range in M_500 of ~10^13-10^15 Msun. We find that the stellar massfraction enclosed in galaxies at R_500 decreases with increasing total mass as M_500^-0.37± 0.04,independent of redshift. Estimating the total gas mass fraction from a recently derived, high quality scaling relation, the total baryon mass fraction(f_500^stars+gas=f_500^stars+f_500^gas) is found to increase by ~25% when M500 increases from <M>=5x10^13 Msun to <M>= 7 x 10^14 Msun. After consideration of a plausible contribution due to intra--cluster light (16% of the total stellar mass), and gas depletion through the hierarchical assembly process (10% of the gas mass), the estimated values of the total baryon mass fraction are still lower than the latest CMB measure of the same quantity (WMAP5), at a significance level of 3.7 sigma for groups of <M>=5x10^13 Msun. The discrepancy decreases towards higher total masses, such that it is 1sigma at <M>= 7x10^14 Msun. We discuss this result in terms of non-gravitational processes such as feedback and filamentary heating.
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