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The Implications of the NewZ = 0 Stellar Models and Yields on the Early Metal Pollution of the Intergalactic Medium

2001/04/17 by C. Abia, I. Domı́nguez, I. Dominguez +5 · 2 citations
Physics and Astronomy · #Astronomy and Astrophysical Research #Galaxies: Formation, Evolution, Phenomena #Stellar, planetary, and galactic studies #astro-ph

paper · pdf · doi:10.1086/321660

30 pages, 6 figures, 2 tables. Accepted in ApJ

arxiv created 2001/04/17 · openalex publication_date 2001/08/10 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/31

Abstract

Motivated by the recent detection of metals in different components of the high-redshift universe and by the abundance ratios measured in the extremely metal-poor stars of our Galaxy, we study the nucleosynthesis constraints that this imposes on an early generation of stars (Population III). To do so we take into account the chemical yields obtained from homogeneous evolutionary calculations of zero-metal stars in the mass range 3 ≲ m / M ☉ ≲ 40 (Limongi et al.; Chieffi et al.). We also consider the role played by metal-free very massive objects ( m > 100 M ☉ ). Using both analytical and numerical chemical evolution models, we confront model predictions from the different choices of the mass function proposed for Population III with the observational constraints. We show that low values of star formation efficiency (<1%) are required so as not to exceed the minimum metallicity ([C/H] ≈ -2.4) measured in the high-redshift systems for any of the initial mass functions (IMFs) proposed. We also show that the observational constraints require Ω sr < 3 × 10 -3 Ω b , confirming previous claims that the possible contribution of the stellar remnants from Population III to the baryonic dark matter is insignificant. At present, however, the scarcity of abundance measurements for high-redshift systems does not permit us to put severe limitations on the nature of the initial mass function for Population III. In fact, overabundances of α-elements with respect to iron of the order of those measured in damped Lyα systems are obtained for any of the IMFs tested. Nevertheless, to account for the very large [C, N/Fe] ratios found in a considerable number of extremely metal-poor stars of our Galaxy, an IMF peaking at the intermediate stellar mass range (4-8 M ☉ ) is needed.

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