2024A&A...691A.128D


Query : 2024A&A...691A.128D

2024A&A...691A.128D - Astronomy and Astrophysics, volume 691A128 (2024/11-1)

S-process nucleosynthesis in chemically peculiar binaries.

DIMOFF A.J., HANSEN C.J., STANCLIFFE R., KUBATOVA B., STATEVA I., KUCINSKAS A. and DOBROVOLSKAS V.

Abstract (from CDS):

Context. Around half of the heavy elements in the Universe are formed through the slow neutron capture (s-) process, which takes place in thermally pulsing asymptotic giant branch (AGB) stars with masses of 1 - 6 M⊙. The nucleosynthetic imprint of the s-process can be studied by observing the material on the surface of binary barium (Ba), carbon (C), CH, and carbon-enhanced metal-poor (CEMP) stars.
Aims. We study the s-process by observing the luminous components of binary systems polluted by a previous AGB companion. Our radial velocity (RV) monitoring program establishes an ongoing collection of binary stars exhibiting enrichment in s-process material for the study of elemental abundances, the production of s-process material, and binary mass transfer.
Methods. From high-resolution optical spectra, we measured RVs for 350 stars and derived stellar parameters for approximately 150 stars using ATHOS. For a subsample of 24 chemically interesting stars, we refined our atmospheric parameters using ionization and excitation balance with the Xiru program. We used the MOOG code to compute one-dimensional local thermodynamic equilibrium (1D-LTE) abundances of carbon, magnesium, s-process elements (Sr, Y, Zr, Mo, Ba, La, Ce, Nd, Pb), and Eu to investigate neutron capture events and stellar chemical composition. We estimated dynamical stellar masses via orbital optimization using Markov chain Monte Carlo techniques in the ELC program, and we compared our results with low-mass AGB models in the FUll-Network Repository of Updated Isotopic Tables & Yields (FRUITY) database.
Results. In our abundance subsample, we find enhancements in s-process material in spectroscopic binaries, a signature of AGB mass transfer. We add the element Mo to the abundance patterns, and for 12 stars we add Pb detections or upper limits, as these are not known in the literature. Computed abundances are in general agreement with the literature. Comparing our abundances to dilution-modified FRUITY yields, we find correlations in s-process enrichment and AGB mass, which are supported by dynamical modeling from RVs.
Conclusions. From our high-resolution observations, we expand heavy element abundance patterns and highlight binarity in our chemically interesting systems. We find trends in s-process element enhancement from AGB stars, and agreement between theoretical and dynamically modeled masses. We investigate evolutionary stages for a small subset of our stars.

Abstract Copyright: © The Authors 2024

Journal keyword(s): nuclear reactions - nucleosynthesis - abundances - stars: abundances - stars: AGB and post-AGB - binaries: spectroscopic - stars: chemically peculiar - stars: low-mass

Simbad objects: 25

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Number of rows : 25
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 TYC 2866-338-1 SB* 03 34 08.4995149872 +40 05 42.234819396   12.48 11.39     ~ 2 0
2 HE 0414-0343 SB* 04 17 16.4631860496 -03 36 31.388697180   12.23 11.04     CEMP-r/s 21 0
3 HD 276679 ** 04 40 06.75024 +42 19 54.5448           F2 6 0
4 HD 31487 SB* 04 59 03.7278166656 +51 56 32.031317148   9.47 8.12     G8IIIBa3 62 0
5 V* CL Cam RS* 05 18 31.0946315760 +75 56 49.326510552   8.50 7.42     G5 36 0
6 V* HR CMa SB* 06 32 46.8731198040 -11 09 58.987412460 8.12 7.35 6.24 5.49 5.01 G9III:Ba3.5 190 0
7 HD 50264 SB* 06 51 12.5032525968 -29 34 32.306464056   9.63 9.05     G1.5II-III:_Ba2_CH0.5 58 0
8 HD 51273 PM* 06 58 20.1775806696 +36 52 38.938420812   8.59 8.12     G0 5 0
9 V* PV UMa SB* 09 03 32.2721549112 +53 06 29.817440280   7.86 6.86     G7III:Ba0.5 78 0
10 BD+41 2150 SB* 11 00 48.5526573816 +40 42 10.560847140   11.2 10.03     C3,1_CH3_Ba4 31 0
11 BD+04 2466 Pe* 11 26 49.1891119944 +03 51 51.641714700   11.22 10.67 10.45   KIIvw 85 0
12 HD 101581 PM* 11 41 02.4684650438 -44 24 18.686737705 9.753 8.833 7.762 7.127 6.584 K4.5Vk: 128 0
13 BSD 56-46 Pe* 11 55 16.5604325976 +28 21 00.735046848   12.48 12.32 11.659 11.296 CEMP-s 16 0
14 HD 103545 Pe* 11 55 27.1610999880 +09 07 45.019860708   9.91 9.20 9.17   KIIvw 78 0
15 * omi Vir SB* 12 05 12.5318326945 +08 43 58.866875781 5.75 5.11 4.12 3.38 2.89 G8IIICN0.5CH1Ba1 301 0
16 HD 105671 PM* 12 09 54.9817584989 -46 12 30.211324851 10.648 9.573 8.438 7.777 7.239 K4Vk: 86 0
17 TYC 8258-1189-1 * 12 58 58.0559592456 -50 44 37.731169788   11.778 10.847     ~ 8 0
18 HD 116514 SB* 13 23 36.2281776816 +33 22 25.190524380   9.97 9.30     G4V 24 0
19 BD-19 3868 SB* 14 23 55.4929288104 -20 21 04.010397516   11.937 10.674     ~ 6 0
20 HD 135148 SB* 15 13 17.4566472168 +12 27 25.533915552   10.87 9.39 8.97   CEMP-s 100 0
21 HD 196673 ** 20 37 44.3242645 +33 21 59.371434           K0pBa+G5III 61 0
22 CD-62 1346 Pe* 21 06 02.9219229360 -61 33 44.645403600   10.55 9.85 9.56 9.027 CEMP-s 70 0
23 HD 209621 SB* 22 04 25.1430497160 +21 03 08.991263304   10.41 8.86     C-H3III: 111 0
24 V* HR Peg S* 22 54 35.6272159944 +16 56 30.606025560 9.970 8.160 6.360     S4+/1+ 137 0
25 TYC 2250-1047-1 * 23 27 43.0145801280 +23 40 03.416244744   12.41 11.67     ~ 3 0

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