s-Process in low-metallicity stars – I. Theoretical predictions

• Published in: Monthly notices of the Royal Astronomical Society 2010-05, Vol.404 (3), p.1529-1544
• Main Authors: Bisterzo, S., Gallino, R., Straniero, O., Cristallo, S., Käppeler, F.
• Format: Article
• Language: English
• Subjects: Abundance; abundances; Astronomy; Astrophysics; Asymptotic properties; Carbon; Chemical elements; Earth, ocean, space; Evolutionary; Exact sciences and technology; Metallicity; Neutron sources; Nuclear physics; nuclear reactions; nuclear reactions, nucleosynthesis, abundances; nucleosynthesis; Spreads; Star & galaxy formation; Stars; Stars & galaxies; stars: carbon; stars: Population II
• ISSN: 0035-8711; 1365-2966
• DOI: 10.1111/j.1365-2966.2010.16369.x

A large sample of carbon-enhanced metal-poor stars enriched in s-process elements (CEMP-s) have been observed in the Galactic halo. These stars of low mass (M∼ 0.9 M⊙) are located on the main-sequence or the red-giant phase, and do not undergo third dredge-up (TDU) episodes. The s-process enhancement is most plausibly due to accretion in a binary system from a more massive companion when on the asymptotic giant branch (AGB) phase (now a white dwarf). In order to interpret the spectroscopic observations, updated AGB models are needed to follow in detail the s-process nucleosynthesis. We present nucleosynthesis calculations based on AGB stellar models obtained with Frascati Raphson-Newton Evolutionary Code (franec) for low initial stellar masses and low metallicities. For a given metallicity, a wide spread in the abundance of the s-process elements is obtained by varying the amount of 13C and its profile in the pocket, where the 13C(α, n)16O reaction is the major neutron source, releasing neutrons in radiative conditions during the interpulse phase. We also account for the second neutron source 22Ne(α, n)25Mg, partially activated during convective thermal pulses. We discuss the surface abundance of elements from carbon to bismuth, for AGB models of initial masses M= 1.3–2 M⊙, low metallicities ([Fe/H] from −1 down to −3.6) and for different 13C-pocket efficiencies. In particular, we analyse the relative behaviour of the three s-process peaks: light-s (ls at magic neutron number N= 50), heavy-s (hs at N= 82) and lead (N= 126). Two s-process indicators, [hs/ls] and [Pb/hs], are needed in order to characterize the s-process distribution. In the on-line material, we provide a set of data tables with surface predictions. Our final objective is to provide a full set of theoretical models of low-mass low-metallicity s-process-enhanced stars. In a forthcoming paper, we will test our results through a comparison with observations of CEMP-s stars.