2002/12/31 by Neta A. Bahcall, Paul Bode · 4 citations
Physics and Astronomy · #Astronomy and Astrophysical Research #Cosmology and Gravitation Theories #Galaxies: Formation, Evolution, Phenomena #astro-ph
paper · pdf · doi:10.1086/375503
published as Astrophys.J. 588 (2003) L1-L4 · 12 pages including 3 figures; updated to match published version
openalex publication_date 2003/03/31 · arxiv created 2003/04/16 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/31
We determine the linear amplitude of mass fluctuations in the universe, σ 8 , from the abundance of massive clusters at redshifts z = 0.5-0.8. The evolution of massive clusters depends exponentially on the amplitude of mass fluctuations and thus provides a powerful measure of this important cosmological parameter. The relatively high abundance of massive clusters observed at z > 0.5 and the relatively slow evolution of their abundance with time suggest a high amplitude of mass fluctuations: σ 8 = 0.9 (±10%) for Ω m = 0.4, increasing slightly to σ 8 = 0.95 for Ω m = 0.25 and σ 8 = 1.0 for Ω m = 0.1 (flat cold dark matter models). We use the cluster abundance observed at z = 0.5-0.8 to derive a normalization relation from the high-redshift clusters, which is only weakly dependent on Ω m : σ 8 Ω = 0.78 ± 0.08. When combined with recent constraints from the present-day cluster mass function, σ 8 Ω = 0.33 ± 0.03, we find σ 8 = 0.98 ± 0.1 and Ω m = 0.17 ± 0.05. Low-σ 8 values (≲0.7) are unlikely; they produce an order-of-magnitude fewer massive clusters than observed.