Stellar and Total Baryon Mass Fractions in Groups and Clusters Since Redshift 1
- Creators
- Giodini, S.
- Pierini, D.
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Finoguenov, A.
- Pratt, G. W.
- Boehringer, H.
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Leauthaud, A.
- Guzzo, L.
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Aussel, H.
- Bolzonella, M.
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Capak, P.
- Elvis, M.
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Hasinger, G.
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Ilbert, O.
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Kartaltepe, J. S.
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Koekemoer, A. M.
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Lilly, S. J.
- Massey, R.
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McCracken, H. J.
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Rhodes, J.
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Salvato, M.
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Sanders, D. B.
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Scoville, N. Z.
- Sasaki, S. S.
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Smolčić, V.
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Taniguchi, Y.
- Thompson, D.
- COSMOS Collaboration
Abstract
We 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 with a robust, analogous determination of the total and stellar mass inside R_(500). The total sample of 118 groups and clusters with z ≤ 1 spans a range in M_(500) of ~10^(13)-10^(15) M_☉. We find that the stellar mass fraction associated with galaxies at R_(500) decreases with increasing total mass as M^(–0.37 ± 0.04)_(500), independent of redshift. Estimating the total gas mass fraction from a recently derived, high-quality scaling relation, the total baryon mass fraction (f^(stars+gas)_(500) = f^(stars)_(500) + f^(gas)_(500)) is found to increase by ~25%, when M_(500) increases from = 5 × 10^(13) M_☉ to = 7 × 10^(14) M_☉. After consideration of a plausible contribution due to intracluster light (11%-22% 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 3.3σ for groups of = 5 × 10^(13) M_☉. The discrepancy decreases toward higher total masses, such that it is 1σ at = 7 × 10^(14) M_☉. We discuss this result in terms of nongravitational processes such as feedback and filamentary heating.
Additional Information
© 2009 American Astronomical Society. Received 2008 December 16, accepted for publication 2009 July 21. Published 2009 September 3. The authors thank the anonymous referee for her/his valuable comments, which led to a significant improvement of the paper. We acknowledge the contributions of the entire COSMOS collaboration; more information on the COSMOS survey are available at http://www.astr.caltech.edu/∼cosmos. This research was supported by the DFG Cluster of Excellence Origin and Structure of the Universe (http://www.universe-cluster.de). D.P. acknowledges support by the German Deutsches Zentrum für Luft- und Raumfahrt, DLR project number 50 OR 0405.Attached Files
Published - Giodini2009p5939Astrophys_J.pdf
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Additional details
- Eprint ID
- 16187
- Resolver ID
- CaltechAUTHORS:20091006-134828649
- Deutsche Forschungsgemeinschaft (DFG)
- Deutsches Zentrum für Luft- und Raumfahrt (DLR)
- 50 OR 0405
- Created
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2009-10-06Created from EPrint's datestamp field
- Updated
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2021-11-08Created from EPrint's last_modified field
- Caltech groups
- COSMOS, Infrared Processing and Analysis Center (IPAC)