1996/12/17 by Nickolay Y. Gnedin, Jeremiah P. Ostriker · 3 citations
Physics and Astronomy · #Cosmology and Gravitation Theories #Galaxies: Formation, Evolution, Phenomena #Stellar, planetary, and galactic studies #astro-ph
paper · pdf · doi:10.1086/304548
published as Astrophys.J. 486 (1997) 581 · submitted to ApJ
arxiv created 1996/12/17 · openalex publication_date 1997/09/10 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/04
We simulate a plausible cosmological model in considerable physical and numerical detail through the successive phases of reheating (at 10 ≲ z ≲ 20) and reionization at z ≈ 7. We assume an efficiency of high-mass star formation appropriate to leave the universe, after it becomes transparent, with an ionizing background J 21 ≈ 0.4 (at z = 4), near (and perhaps slightly below) the observed value. Since the same stars produce the ionizing radiation and the first generation of heavy elements, a mean metallicity of ⟨ Z / Z ☉ ⟩ ~ 1/200 is produced in this early phase, but there is a large variation about this mean, with the high density regions having Z / Z ☉ ≈ 1/30 and the low density regions (or the Lyα forest with N H I ≲ 10 13.5 cm 2 ) having essentially no metals. When it occurs, reionization is very rapid (phase change-like), which will leave a signature that may be detectable by very large area meter-wavelength radio instruments. Also, the background UV radiation field will show a sharp drop of ~10 -3 from 1 to 4 ryd because of absorption edges. The simulated volume is too small to form L * galaxies, but the smaller objects that are found in the simulation obey the Faber-Jackson relation. In order to explore theoretically this domain of "the end of the dark ages" quantitatively, numerical simulations must have a mass resolution of the order of 10 4.5 M ☉ in baryons, have high spatial resolution (≲1 kpc) to resolve strong clumping, and allow for detailed and accurate treatment of both the radiation field and atomic/molecular physics.