Deuterium, lithium and the density of the Universe
The main outcome of the primordial nucleosynthesis is the ability to account for the abundances of D, ^sup 3^He, ^sup 4^He and ^sup 7^Li with the proper choice of the nuclear density parameter ω^sub B^. The relative advantages/disadvantages of D and ^sup 7^Li as the proper `baryometer' are disc...
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Veröffentlicht in: | Astrophysics and space science 1999-07, Vol.265 (1-4), p.23-27 |
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description | The main outcome of the primordial nucleosynthesis is the ability to account for the abundances of D, ^sup 3^He, ^sup 4^He and ^sup 7^Li with the proper choice of the nuclear density parameter ω^sub B^. The relative advantages/disadvantages of D and ^sup 7^Li as the proper `baryometer' are discussed. In favour of D, the main arguments are the relative simplicity of the formation/destruction schema, but this is challenged by the large uncertainties on the choice of its actual `primordial' abundance and on the galactic evolution scheme. In favour of ^sup 7^Li there are the confirmation of the so called `Spite plateau' and the observation of ^sup 6^Li at the surface of at least one (may be two) Population II stars, but the paucity of such stars such as the possibility of scenarios in which the ^sup 7^Li abundance could be affected even in these stars cannot be overlooked.[PUBLICATION ABSTRACT] |
doi_str_mv | 10.1023/A:1002123614254 |
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The relative advantages/disadvantages of D and ^sup 7^Li as the proper `baryometer' are discussed. In favour of D, the main arguments are the relative simplicity of the formation/destruction schema, but this is challenged by the large uncertainties on the choice of its actual `primordial' abundance and on the galactic evolution scheme. In favour of ^sup 7^Li there are the confirmation of the so called `Spite plateau' and the observation of ^sup 6^Li at the surface of at least one (may be two) Population II stars, but the paucity of such stars such as the possibility of scenarios in which the ^sup 7^Li abundance could be affected even in these stars cannot be overlooked.[PUBLICATION ABSTRACT]</description><identifier>ISSN: 0004-640X</identifier><identifier>EISSN: 1572-946X</identifier><identifier>DOI: 10.1023/A:1002123614254</identifier><language>eng</language><publisher>Dordrecht: Springer Nature B.V</publisher><subject>Astrophysics ; Cosmology ; Deuterium ; Lithium ; Stars & galaxies ; Universe</subject><ispartof>Astrophysics and space science, 1999-07, Vol.265 (1-4), p.23-27</ispartof><rights>Kluwer Academic Publishers 1999</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>315,782,786,27931,27932</link.rule.ids></links><search><creatorcontrib>Audouze, Jean</creatorcontrib><title>Deuterium, lithium and the density of the Universe</title><title>Astrophysics and space science</title><description>The main outcome of the primordial nucleosynthesis is the ability to account for the abundances of D, ^sup 3^He, ^sup 4^He and ^sup 7^Li with the proper choice of the nuclear density parameter ω^sub B^. The relative advantages/disadvantages of D and ^sup 7^Li as the proper `baryometer' are discussed. In favour of D, the main arguments are the relative simplicity of the formation/destruction schema, but this is challenged by the large uncertainties on the choice of its actual `primordial' abundance and on the galactic evolution scheme. 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subjects | Astrophysics Cosmology Deuterium Lithium Stars & galaxies Universe |
title | Deuterium, lithium and the density of the Universe |
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