2024A&A...684A.206C


Query : 2024A&A...684A.206C

2024A&A...684A.206C - Astronomy and Astrophysics, volume 684A206 (2024/4-1)

The intermediate neutron capture process V. The i-process in AGB stars with overshoot.

CHOPLIN A., SIESS L., GORIELY S. and MARTINET S.

Abstract (from CDS):

Context. The intermediate neutron capture process (i-process) can develop during proton ingestion events (PIE), potentially during the early stages of low-mass low-metallicity asymptotic giant branch (AGB) stars.
Aims. We examine the impact of overshoot mixing on the triggering and development of i-process nucleosynthesis in AGB stars of various initial masses and metallicities.
Methods. We computed AGB stellar models, with initial masses of 1, 2, 3, and 4 M⊙ and metallicities in the -2.5 ≤ [Fe/H] ≤ 0 range, using the stellar evolution code STAREVOL with a network of 1160 nuclei coupled to the transport equations. We considered different overshooting profiles below and above the thermal pulses, and below the convective envelope.
Results. The occurrence of PIEs is found to be primarily governed by the amount of overshooting at the top of pulse (ftop) and to increase with rising ftop. For ftop = 0, 0.02, 0.04, and 0.1, we find that 0%, 6%, 24%, and 86% of our 21 AGB models with -2 < [Fe/H] < 0 experience a PIE, respectively. Variations of the overshooting parameters during a PIE leads to a scatter on abundances of 0.5 - 1 dex on elements, with 36 < Z < 56; however, this barely impacts the production of elements with 56 < Z < 80, which therefore appear to be a reliable prediction of our models. Actinides are only produced if the overshooting at the top of pulse is small enough. We also find that PIEs leave a 13C-pocket at the bottom of the pulse that can give rise to an additional radiative s-process nucleosynthesis. In the case of the 2 M⊙ models with [Fe/H] = -1 and -0.5, it produces a noticeable mixed i + s chemical signature at the surface. Finally, the chemical abundance patterns of 22 observed r/s-stars candidates (18 dwarfs or giants and 4 post-AGB) with -2 < [Fe/H] < -1 are found to be in reasonable agreement with our AGB model predictions. The binary status of the dwarfs/giants being unclear, we suggest that these stars have acquired their chemical pattern either from the mass transfer of a now-extinct AGB companion or from an early generation AGB star that polluted the natal cloud.
Conclusions. The occurrence of PIEs and the development of i-process nucleosynthesis in AGB stars remains sensitive to the overshooting parametrization. A high (yet realistic) ftop value triggers PIEs at (almost) all metallicities. The existence of r/s-stars at [Fe/H] ≃ -1 is in favour of an i-process operating in AGB stars up to this metallicity. Stricter constraints from multi-dimensional hydrodynamical models on overshoot coefficients could deliver new insights into the contribution of AGB stars to heavy elements in the Universe.

Abstract Copyright: © The Authors 2024

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

Simbad objects: 22

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Number of rows : 22
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 2MASS J00045537-2424193 * 00 04 55.3702511976 -24 24 19.266450696   14.209 13.737 13.430 13.128 ~ 18 0
2 OGLE SMC-LPV-4910 pA* 00 44 41.1035011488 -73 21 36.123508332   17.06 15.61 15.44 14.515 G:I 30 0
3 HD 5223 SB* 00 54 13.6098985200 +24 04 01.515842760   9.87 8.47     C-H2IIIb: 126 0
4 HE 0507-1653 SB* 05 09 16.5603215496 -16 50 04.688981556   13.633 12.507 12.002 11.579 CEMP-s 26 0
5 OGLE LMC-LPV-39792 LP* 05 18 48.8624065560 -70 02 47.086220796 18.692 17.142 15.429 14.31 13.852 F4Ib-II(e) 19 0
6 OGLE LMC-LPV-43685 pA* 05 20 43.8870629914 -69 23 41.139112840 17.618 16.515 15.075 13.92 13.887 F5Ib(e) 23 0
7 OGLE LMC-LPV-68005 LP* 05 32 50.7147024408 -71 39 25.723947636 17.985 16.533 15.069   13.803 F6Ia 18 0
8 HE 1120-2122 SB* 11 23 18.6203961912 -21 38 32.303797404   13.303 11.795 11.126 10.568 CEMP-rs 14 0
9 HD 106038 PM* 12 12 01.3688687080 +13 15 40.618559661 10.45 10.630 10.162 9.851 9.539 F6wl 204 0
10 RAVE J130200.0-084328 Pe* 13 01 59.9615903376 -08 43 28.783996932   12.978 11.884 11.677   CEMP 12 0
11 2MASS J13364604+4503086 Pe* 13 36 46.0325838312 +45 03 08.641824120   14.57 13.8 13.401 12.974 CEMP-r/s 19 0
12 HD 126681 PM* 14 27 24.9094012952 -18 24 40.454425566   9.939 9.535     G3V 208 0
13 2MASS J16510881+5712277 Pe* 16 51 08.8035670560 +57 12 27.769041180   14.80 14.4 13.986 13.672 CEMP-s 20 0
14 HD 166161 PM* 18 09 40.6841536776 -08 46 45.603012144 9.53 9.13 8.16     G0wF0 148 0
15 HD 166913 PM* 18 16 25.6832938176 -59 24 11.239435980   8.66 8.23     F5/7Vw 142 0
16 BPS CS 22880-0074 Pe* 20 46 03.2162534976 -20 59 14.110203840   13.84 13.27 12.770 12.382 CEMP-s 49 0
17 HD 206983 LP? 21 46 09.3423868872 -15 14 39.766213896   11.1 9.45     CEMP-s 50 1
18 HE 2144-1832 SB* 21 46 54.6639160128 -18 18 15.587038476   12.651 10.97 10.471 9.860 CEMP-s 16 0
19 TYC 6953-510-1 * 21 51 52.4886187848 -22 56 05.691899364   11.859 10.95 10.71   ~ 18 0
20 HD 209621 SB* 22 04 25.1430497160 +21 03 08.991263304   10.41 8.86     C-H3III: 111 0
21 BPS CS 22887-0048 Pe* 22 46 44.6216572248 -11 08 42.414994716   13.26 12.87 12.588 12.31 CEMP-s 29 0
22 BPS CS 29513-0032 Pe* 23 22 19.0938404592 -39 44 24.309461652 14.757 14.97 14.47     ~ 19 0

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