2021A&A...648A.119C


Query : 2021A&A...648A.119C

2021A&A...648A.119C - Astronomy and Astrophysics, volume 648A119-119 (2021/4-1)

The intermediate neutron capture process. I. Development of the i-process in low-metallicity low-mass AGB stars.

CHOPLIN A., SIESS L. and GORIELY S.

Abstract (from CDS):


Context. Results from observations report a growing number of metal-poor stars showing an abundance pattern midway between the s- and r-processes. These so-called r/s-stars raise the need for an intermediate neutron capture process (i-process), which is thought to result from the ingestion of protons in a convective helium-burning region, but whose astrophysical site is still largely debated.
Aims. We investigate whether an i-process during the asymptotic giant branch (AGB) phase of low-metallicity low-mass stars can develop and whether it can explain the abundances of observed r/s-stars.
Methods. We computed a 1M☉ model at [Fe/H] = -2.5 with the stellar evolution code STAREVOL, using a nuclear network of 1091 species (at maximum) coupled to the transport processes. The impact of the temporal and spatial resolutions on the resulting abundances was assessed. We also identified key elements and isotopic ratios that are specific to i-process nucleosynthesis and carried out a detailed comparison between our model and a sample of r/s-stars.
Results. At the beginning of the AGB phase, during the third thermal pulse, the helium driven convection zone is able to penetrate the hydrogen-rich layers. The subsequent proton ingestion leads to a strong neutron burst with neutron densities of ∼4.3x1014cm–3 at the origin of the synthesis of i-process elements. The nuclear energy released by proton burning in the helium-burning convective shell strongly affects the internal structure: the thermal pulse splits and after approximately ten years the upper part of the convection zone merges with the convective envelope. The surface carbon abundance is enhanced by more than 3 dex. This leads to an increase in the opacity, which triggers a strong mass loss and prevents any further thermal pulse. Our numerical tests indicate that the i-process elemental distribution is not strongly affected by the temporal and spatial resolution used to compute the stellar models, but typical uncertainties of ±0.3dex on individual abundances are found. We show that specific isotopic ratios of Ba, Nd, Sm, and Eu can represent good tracers of i-process nucleosynthesis. Finally, an extended comparison with 14 selected r/s-stars show that the observed composition patterns can be well reproduced by our i-process AGB model.
Conclusions. A rich i-process nucleosynthesis can take place during the early AGB phase of low-metallicity low-mass stars and explain the elemental distribution of most of the r/s-stars, but cannot account for the high level of enrichment of the giant stars in a scenario involving pollution by a former AGB companion.

Abstract Copyright: © ESO 2021

Journal keyword(s): nuclear reactions - nucleosynthesis - abundances - stars: AGB and post-AGB

Errata: erratum vol. 662, art. C3 (2022)

Simbad objects: 15

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Number of rows : 15
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 224959 SB* 00 02 08.0214788256 -02 49 12.232785144   10.6 9.6     CEMP-rs 104 0
2 BPS CS 31062-0050 Pe* 00 30 31.0646803224 -12 05 10.877225064   13.7 13.05 12.681 12.309 CEMP-r/s 70 0
3 CD-24 266 BS* 00 40 47.9313619824 -24 07 34.183333668   12.955 12.656 12.441 12.216 CEMP-s 100 0
4 HE 0243-3044 Pe* 02 45 16.4464212312 -30 32 02.118309504   17.11 16.10     CEMP-rs 15 0
5 HE 0338-3945 Pe* 03 39 55.0068570984 -39 35 42.902896452   15.753 15.333 15.098 14.787 CEMP-r/s 42 0
6 UCAC4 407-057901 Pe* 14 07 42.9724778472 -08 36 14.381637516   14.910 14.099 13.929 13.171 CEMP-s 14 0
7 HE 1429-0551 Pe* 14 32 31.2973339296 -06 05 00.201354252   14.015 12.606 11.995 11.537 CEMP-s 29 0
8 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 985 0
9 HD 145777 SB* 16 13 13.8686004888 -15 12 01.247063688   11.55 10.31     CEMP-rs 36 0
10 2MASS J19280402-5924264 Pe* 19 28 04.0285893888 -59 24 26.474182668   15.15 14.29 13.808 13.375 CEMP-rs 20 0
11 HD 187861 SB* 19 56 26.9442832128 -65 22 08.014212084   10.42 9.18     CEMP-rs 70 0
12 HE 2122-4707 Pe* 21 25 44.5036856403 -46 54 11.705888852   16.163 15.243 15.212   CEMP-r/s 8 0
13 HE 2134-3940 Pe* 21 37 45.7673945880 -39 27 22.313379600   13.790 12.660 12.160 11.760 KIIvw 88 0
14 HE 2148-1247 Pe* 21 51 17.9096426016 -12 33 41.557315896   15.266 14.740 14.582   CEMP-r/s 51 0
15 HE 2258-6358 Pe* 23 01 48.6559441632 -63 42 25.117355556   15.42 14.30 14.07   CEMP-s 14 0

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