2011
DOI: 10.1088/0004-637x/742/2/121
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Three-Dimensional Hydrodynamical Simulations of a Proton Ingestion Episode in a Low-Metallicity Asymptotic Giant Branch Star

Abstract: We use the 3D stellar structure code djehuty to model the ingestion of protons into the intershell convection zone of a 1 M ⊙ asymptotic giant branch star of metallicity Z = 10 −4 . We have run two simulations: a low resolution one of around 300,000 zones, and a high resolution one consisting of 2,000,000 zones. Both simulations have been evolved for about 4 hours of stellar time. We observe the existence of fast, downward flowing plumes that are able to transport hydrogen into close proximity to the helium bu… Show more

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Cited by 100 publications
(165 citation statements)
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“…There are as yet no detailed models of this process for low-metallicity AGB stars, although PIE events have been identified as a a possible physical site (the i-process, Cowan & Rose 1977;Herwig et al 2011). Overshoot leading to PIEs is uncertain, but known to be favoured in AGB stars of mass ∼1 M and [Fe/H] < 2 (Fujimoto et al 1990;Campbell & Lattanzio 2008;Cristallo et al 2009;Lugaro et al 2012) with recent 3D models supporting these results (Stancliffe et al 2011;Herwig et al 2014;Woodward et al 2015). We stress that one-dimensional hydrostatic models of PIE events with artificial proton distributions like those presented here are not expected to describe the ingestion and the mixing correctly, and this may have a strong effect on the resulting abundance patterns.…”
Section: Discussionmentioning
confidence: 91%
“…There are as yet no detailed models of this process for low-metallicity AGB stars, although PIE events have been identified as a a possible physical site (the i-process, Cowan & Rose 1977;Herwig et al 2011). Overshoot leading to PIEs is uncertain, but known to be favoured in AGB stars of mass ∼1 M and [Fe/H] < 2 (Fujimoto et al 1990;Campbell & Lattanzio 2008;Cristallo et al 2009;Lugaro et al 2012) with recent 3D models supporting these results (Stancliffe et al 2011;Herwig et al 2014;Woodward et al 2015). We stress that one-dimensional hydrostatic models of PIE events with artificial proton distributions like those presented here are not expected to describe the ingestion and the mixing correctly, and this may have a strong effect on the resulting abundance patterns.…”
Section: Discussionmentioning
confidence: 91%
“…This point is very relevant, as it has recently been suggested that α should vary during the evolution of the star - Meakin & Arnett (2007). Moreover, it is possible that mixing length theory cannot adequately describe the convection of the actual star - Stancliffe et al (2011). Alternatively, if we could find some observational constraints on these models, we might be able to use these to discriminate between different convection theories or different values of α for this phase of the evolution.…”
Section: Discussionmentioning
confidence: 98%
“…Splitting of the HeCZ (shell) is also found in PIE resulting from very late thermal pulses in post-AGB stars (Herwig 2001;Althaus et al 2005) and in simulations of the early phases of the TP-AGB in very metal-poor stars (Fujimoto et al 2000;Serenelli 2006;Cristallo et al 2009). On the other hand, recent hydrodynamic 3-dimensional simulations of the TP-AGB phase for a low-mass star (Stancliffe et al 2011) have not shown splitting of the HeCZ, although the authors argued this might be an artifact of the low resolution used in the calculations.…”
Section: Figmentioning
confidence: 96%