2015
DOI: 10.1093/mnras/stv1489
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Evolution and nucleosynthesis of helium-rich asymptotic giant branch models

Abstract: There is now strong evidence that some stars have been born with He mass fractions as high as Y ≈ 0.40 (e.g., in ω Centauri). However, the advanced evolution, chemical yields, and final fates of He-rich stars are largely unexplored. We investigate the consequences of He-enhancement on the evolution and nucleosynthesis of intermediatemass asymptotic giant branch (AGB) models of 3, 4, 5, and 6 M with a metallicity of Z = 0.0006 ([Fe/H] ≈ −1.4). We compare models with He-enhanced compositions (Y = 0.30, 0.35, 0.4… Show more

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Cited by 24 publications
(47 citation statements)
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References 118 publications
(145 reference statements)
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“…Most heavy elements, X, are only moderately overabundant, with 0<[X/Fe]<1. We compare this pattern with six sets of low-metallicity ([Fe/H]=−1.4) AGB nucleosynthesis yields, with Y=0.24, taken from and Shingles et al (2015). Several example fits are shown.…”
Section: Comparison With Agb Nucleosynthesis Predictionsmentioning
confidence: 99%
See 1 more Smart Citation
“…Most heavy elements, X, are only moderately overabundant, with 0<[X/Fe]<1. We compare this pattern with six sets of low-metallicity ([Fe/H]=−1.4) AGB nucleosynthesis yields, with Y=0.24, taken from and Shingles et al (2015). Several example fits are shown.…”
Section: Comparison With Agb Nucleosynthesis Predictionsmentioning
confidence: 99%
“…We use the low-metallicity AGB evolution and nucleosynthesis models from and Shingles et al (2015). These models were calculated with an initial metallicity of Z=0.0006 ([Fe/H] =−1.4), which is close to the derived metallicity of HD94028.…”
Section: Agb Modelsmentioning
confidence: 99%
“…The models of Gallino et al (1998) (and follow-up studies by, e.g., Bisterzo et al 2010Bisterzo et al , 2011Liu et al 2015) are calculated by including some 13 C in the intershell and exploring a large variety of extents and abundance profiles. The models of, e.g., Goriely & Mowlavi (2000); Lugaro et al (2012); Fishlock et al (2014); Shingles et al (2015); instead are calculated including a PMZ by means of an artificial mixing profile, driving the mixing of protons that subsequently produce a 13 C abundance profile. The mixing is modelled using an exponential function where the exponent is a linear function of the mass ("standard" case, see details in Sec.…”
Section: Current Models For the Formation Of 13 C Pocketsmentioning
confidence: 99%
“…We note that CONe cores are found over a large variety of metallicities and also for a range of helium enrichments (Shingles et al 2015). In any case, a narrow mass range would allow us to explain at most a few percent of the observed SNIa (Meng & Podsiadlowski 2014).…”
Section: Introductionmentioning
confidence: 76%