2024A&A...687A.260R


Query : 2024A&A...687A.260R

2024A&A...687A.260R - Astronomy and Astrophysics, volume 687A260 (2024/7-1)

The impact of overshoot on the i-process in AGB stars.

REMPLE B.A., BATTICH T. and WEISS A.

Abstract (from CDS):

Context. The production of neutron-rich elements at neutron densities intermediate to those of the s- and r-processes, the so-called i-process, has been identified as possibly being responsible for the observed abundance pattern found in certain carbon-enhanced metal-poor (CEMP) stars. The production site may be low-metallicity stars on the asymptotic giant branch (AGB) where the physical processes during the thermal pulses are not well known.
Aims. We investigate the impact of overshoot from various convective boundaries during the AGB phase on proton ingestion events (PIEs) and the neutron densities as a necessary precondition for the i-process as well as on the structure and continued evolution of the models.
Methods. We therefore analyzed models of a 1.2 M⊙, Z = 5 × 10–5 star. A fiducial model without overshoot on the AGB (overshoot was applied during the pre-AGB evolution) serves as a reference. The same model was then run with various overshoot values and the resulting models were compared to one another. Light element nucleosynthesis is also discussed. Additionally, we introduce a new timescale argument to predict PIE occurrence to discriminate between a physical and a numerical reason for a nonoccurrence. A comparison to observations as well as previous studies was conducted before finally presenting the most promising choice of overshoot parameters for the occurrence of the i-process in low-mass, low-metallicity models.
Results. The fiducial model reveals high neutron densities and a persistent split of the pulse-driven convection zone (PDCZ). Overshoot from the PDCZ results in either temporary or permanent remerging of the split PDCZ, influencing the star's structure and evolution. While both overshoot and non-overshoot models exhibit PIEs generating neutron densities suitable for the i-process, they lead to varied C/O and N/O ratios and notable Li enhancements. Comparison with previous studies and observations of CEMP-r/s stars suggests that while surface enhancements in our models may be exaggerated, abundance ratios align well. Though, for high values of overshoot from the PDCZ the agreement becomes worse.

Abstract Copyright: © The Authors 2024

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

Simbad objects: 29

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Number of rows : 29
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 HE 0017+0055 Pe* 00 20 21.6000581352 +01 12 06.817571136   12.991 11.66 10.773 10.186 CEMP-rs 30 0
3 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
4 CD-24 266 BS* 00 40 47.9313619824 -24 07 34.183333668   12.955 12.656 12.441 12.216 CEMP-s 100 0
5 SB 960 Pe* 00 44 03.5698629048 -13 55 26.268999384   12.69 12.15 11.806 11.483 CEMP-s 114 0
6 HD 5223 SB* 00 54 13.6098985200 +24 04 01.515842760   9.87 8.47     C-H2IIIb: 126 0
7 HE 0058-0244 Pe* 01 00 53.0234702616 -02 28 19.950391884   14.42 13.73 13.331 12.942 CEMP-r/s 40 0
8 HE 0151-0341 SB* 01 53 43.3049091528 -03 27 14.456628576   14.67 13.40   12.521 CEMP-rs 11 0
9 HE 0243-3044 Pe* 02 45 16.4464212312 -30 32 02.118309504   17.11 16.10     CEMP-rs 15 0
10 HE 0319-0215 SB* 03 21 46.2603171576 -02 04 33.952124424   15.03 13.60   12.603 CEMP-rs 14 0
11 BPS CS 29526-0110 Pe* 03 27 43.6392396600 -23 00 29.924362260   13.71 13.35 13.116 12.834 CEMP-r/s 54 0
12 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
13 HD 76396 SB* 08 57 58.9267711584 +51 25 47.661787776   9.96 8.85 8.5   C-H2IV: 69 0
14 HE 1120-2122 SB* 11 23 18.6203961912 -21 38 32.303797404   13.303 11.795 11.126 10.568 CEMP-rs 14 0
15 HE 1418+0150 SB* 14 21 01.1688766320 +01 37 17.834854152   13.7 12.205 11.335 10.936 CEMP-s 15 0
16 HE 1429-0551 Pe* 14 32 31.2973339296 -06 05 00.201354252   14.015 12.606 11.995 11.537 CEMP-s 29 0
17 HD 145777 SB* 16 13 13.8686004888 -15 12 01.247063688   11.55 10.31     CEMP-rs 36 0
18 ATO J256.8913+58.8499 RR* 17 07 33.9318852312 +58 50 59.711493732   16.209 15.635 15.977   F5kA2Bapec 35 0
19 V* V4334 Sgr CV* 17 52 32.69352 -17 41 08.0160           F2Ia 390 0
20 HD 187216 Pe* 19 24 18.3437183760 +85 21 57.189325176   11.2 9.56     C3,3_CH5: 78 2
21 2MASS J19280402-5924264 Pe* 19 28 04.0285893888 -59 24 26.474182668   15.15 14.29 13.808 13.375 CEMP-rs 20 0
22 HD 187861 SB* 19 56 26.9442832128 -65 22 08.014212084   10.42 9.18     CEMP-rs 70 0
23 HD 196944 SB* 20 40 46.0815001992 -06 47 50.604476604   9.01 8.40 8.08   CEMP-rs 117 0
24 BPS CS 22898-0027 Pe* 21 05 45.0996805992 -18 36 57.501493128   13.26 12.76 12.476 12.094 CEMP-r/s 88 0
25 HE 2134-3940 Pe* 21 37 45.7673945880 -39 27 22.313379600   13.790 12.660 12.160 11.760 KIIvw 88 0
26 HE 2148-1247 Pe* 21 51 17.9096426016 -12 33 41.557315896   15.266 14.740 14.582   CEMP-r/s 51 0
27 HD 209621 SB* 22 04 25.1430497160 +21 03 08.991263304   10.41 8.86     C-H3III: 111 0
28 HE 2258-6358 Pe* 23 01 48.6559441632 -63 42 25.117355556   15.42 14.30 14.07   CEMP-s 14 0
29 BPS CS 22949-0008 Pe* 23 16 58.7314762776 -03 20 52.625003208   14.61 14.15 13.858 13.545 CEMP-s 23 0

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