Abstract
In this paper, Ωm refers to the contribution of all clustered matter (including baryons) to the stress-energy density. The mean intracluster gas fraction of X-ray clusters within their hydrostatic regions is derived from recent observational compilations of David, Jones & Forman and White & Fabian. At radii encompassing a mean density 500 times the critical value, the individual sample bi-weight means are moderately (2.4σ) discrepant; revising binding masses with a virial relation calibrated by numerical simulations removes the discrepancy and results in a combined sample mean and standard error f̄gas(r500) = (0.060 ± 0.003) h -3/2. For hierarchical clustering models with an extreme physical assumption to maximize cluster gas content, this value constrains the universal ratio of total, clustered-to-baryonic mass Ωm/Ωb ≤ 23.1 h3/2. Combining this with a maximal value of Ωb from primordial nucleosynthesis results in Ωm h1/2 < 0.76. A more physically plausible approach based on low deuterium abundance inferences from quasar absorption spectra and accounting for baryons within cluster galaxies yields an estimate of Ωm h2/3 = 0.30 ± 0.07, with sources of systematic error involved in the derivation providing approximately 30 per cent additional uncertainty. Other effects which could enhance the likelihood of the Einstein-de Sitter case Ωm = 1 are presented, and their observable signatures discussed. © 1997 RAS.
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Evrard, A. E. (1997). The intracluster gas fraction in X-ray clusters: Constraints on the clustered mass density. Monthly Notices of the Royal Astronomical Society, 292(2), 289–297. https://doi.org/10.1093/mnras/292.2.289
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