2016
DOI: 10.1093/mnrasl/slw028
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Evolution of dispersion in the cosmic deuterium abundance

Abstract: Deuterium is created during Big Bang Nucleosynthesis, and, in contrast to the other light stable nuclei, can only be destroyed thereafter by fusion in stellar interiors. In this paper we study the cosmic evolution of the deuterium abundance in the interstellar medium and its dispersion using realistic galaxy evolution models. We find that models that reproduce the observed metal abundance are compatible with observations of the deuterium abundance in the local ISM and z ∼ 3 absorption line systems. In particul… Show more

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Cited by 24 publications
(39 citation statements)
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References 42 publications
(72 reference statements)
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“…We however caution that a high-resolution spectrum with high S/N ratio is necessary to better take into account blends with the Ly-α forest and confirm our measurement. 1 We do not take into account astration of the order of 0.1 dex due to the high metallicity and redshift of our system (see Dvorkin et al 2016). …”
Section: +016mentioning
confidence: 99%
“…We however caution that a high-resolution spectrum with high S/N ratio is necessary to better take into account blends with the Ly-α forest and confirm our measurement. 1 We do not take into account astration of the order of 0.1 dex due to the high metallicity and redshift of our system (see Dvorkin et al 2016). …”
Section: +016mentioning
confidence: 99%
“…In addition, the assumption that D/H=D I/H I is justified in these systems; the ionization correction is expected to be 0.1% (Savin 2002;Cooke & Pettini 2016). Furthermore, galactic chemical evolution models suggest that most of the deuterium atoms in these almost pristine systems are yet to be cycled through many generations of stars; the correction for astration (i.e., the processing of gas through stars) is therefore negligible (see the comprehensive list of references provided by Cyburt et al 2016;Dvorkin et al 2016).…”
Section: Introductionmentioning
confidence: 99%
“…We use the complete formulae for the angular power spectrum, derived in Cusin, Pitrou & Uzan (2017), see also , in our analysis. et al (2016a,b); Dvorkin et al (2018), which we summarize below (see the companion article for extensive explanations). For each model, we compute the GW luminosity L G (z, f G , M G ) of a given galaxy as a function of halo mass M G and redshift z as follows.…”
Section: Astrophysical Building Blocksmentioning
confidence: 90%
“…The overall factor β is used to normalize our model with respect to the number of events observed by LIGO/Virgo. Following Dvorkin et al (2018), the birth rate of binaries with component masses (m, m ≤ m) is R bin (m, m ) = R2(m)R2(m )P (m, m ), where P (m, m ) is a normalized distribution describing the association of mass m and m in a BH binary system.…”
Section: Astrophysical Building Blocksmentioning
confidence: 99%