Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/7187
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dc.contributor.authorCristallo, S-
dc.contributor.authorKarinkuzhi, D-
dc.contributor.authorGoswami, A-
dc.contributor.authorPiersanti, L-
dc.contributor.authorGobrecht, D-
dc.date.accessioned2020-11-17T14:41:04Z-
dc.date.available2020-11-17T14:41:04Z-
dc.date.issued2016-12-20-
dc.identifier.citationThe Astrophysical Journal, Vol. 833, No. 2, 181en_US
dc.identifier.issn0004-637X-
dc.identifier.urihttp://prints.iiap.res.in/handle/2248/7187-
dc.descriptionRestricted Access © The American Astronomical Society http://dx.doi.org/10.3847/1538-4357/833/2/181en_US
dc.description.abstractWe analyze a set of published elemental abundances from a sample of CH stars which are based on high resolution spectral analysis of ELODIE and SUBARU/HDS spectra. All the elemental abundances were derived from local thermodynamic equilibrium analysis using model atmospheres, and thus they represent the largest homogeneous abundance data available for CH stars to date. For this reason, we can use the set to constrain the physics and the nucleosynthesis occurring in low mass asymptotic giant branch (AGB) s.tars. CH stars have been polluted in the past from an already extinct AGB companion and thus show s-process enriched surfaces. We discuss the effects induced on the surface AGB s-process distributions by different prescriptions for convection and rotation. Our reference theoretical FRUITY set fits only part of the observations. Moreover, the s-process observational spread for a fixed metallicity cannot be reproduced. At [Fe/H] > −1, a good fit is found when rotation and a different treatment of the inner border of the convective envelope are simultaneously taken into account. In order to increase the statistics at low metallicities, we include in our analysis a selected number of CEMP stars and, therefore, we compute additional AGB models down to [Fe/H] = −2.85. Our theoretical models are unable to attain the large [hs/ls] ratios characterizing the surfaces of those objects. We speculate on the reasons for such a discrepancy, discussing the possibility that the observed distribution is a result of a proton mixing episode leading to a very high neutron density (the so-called i-process).en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectNuclear reactions, nucleosynthesis, abundancesen_US
dc.subjectPhysical data and processes|en_US
dc.subjectStars: chemically peculiaren_US
dc.subjectStars: evolutionen_US
dc.subjectStars: low-massen_US
dc.titleConstraints of the Physics of Low-Mass AGB Stars from CH and CEMP Starsen_US
dc.typeArticleen_US
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