2018A&A...618A..32K


Query : 2018A&A...618A..32K

2018A&A...618A..32K - Astronomy and Astrophysics, volume 618A32-32 (2018/1-0)

When binaries keep track of recent nucleosynthesis. The Zr-Nb pair in extrinsic stars as an s-process diagnostic.

KARINKUZHI D., VAN ECK S., JORISSEN A., GORIELY S., SIESS L., MERLE T., ESCORZA A., VAN DER SWAELMEN M., BOFFIN H.M.J., MASSERON T., SHETYE S. and PLEZ B.

Abstract (from CDS):

Context. Barium stars are s-process enriched giants. They owe their chemical peculiarities to a past mass transfer phase. During this phase they were polluted by their binary companion, which at the time was an asymptotic giant branch (AGB) star, but is now an extinct white dwarf. Barium stars are thus ideal targets for understanding and constraining the s-process in low- and intermediate-mass AGB stars.
Aims. We derive the abundances of a large number of heavy elements in order to shed light on the conditions of operation of the neutron source responsible for the production of s-elements in the former companions of the barium stars.
Methods. Adopting a recently used methodology, we analyse a sample of eighteen highly enriched barium stars observed with the high-resolution HERMES spectrograph mounted on the Mercator telescope (La Palma). We determine the stellar parameters and abundances using MARCS model atmospheres. In particular, we derive the Nb-Zr ratio which was previously shown to be a sensitive thermometer for the s-process nucleosynthesis. Indeed, in barium stars, 93Zr has fully decayed into mono-isotopic 93Nb, so Nb/Zr is a measure of the temperature-sensitive 93Zr/Zr isotopic ratio.
Results. HD 28159, previously classified as K5III and initially selected to serve as a reference cool K star for our abundance analysis, turns out to be enriched in s-process elements, and as such is a new barium star. Four stars are characterised by high nitrogen abundances, and among those three have high [Nb/Zr] and [hs/ls] ratios. The derived Zr and Nb abundances provide more accurate constraints on the s-process neutron source, identified to be 13C(α, n)16O for barium stars. The comparison with stellar evolution and nucleosynthesis models shows that the investigated barium stars were polluted by a low-mass (M∼2-3M☉) AGB star. HD 100503 is potentially identified as a high metallicity analogue of carbon-enhanced metal-poor star enriched in both r- and s-process elements (CEMP-rs).

Abstract Copyright: © ESO 2018

Journal keyword(s): nuclear reactions - nucleosynthesis - abundances - stars: AGB and post-AGB - binaries: spectroscopic - stars: fundamental parameters

Simbad objects: 43

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Number of rows : 43
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 5424 SB* 00 55 43.9284269928 -27 53 37.262442120   10.558 9.517 9.690   G8II 61 1
2 V* DT Psc Sy* 01 14 04.9051442688 +28 31 46.448476788   8.016 6.347     S3+/2- 129 0
3 HD 7389 Ro* 01 16 11.9019176448 +71 44 37.825280484   7.78 5.86     K5 37 0
4 HD 7733 AB* 01 18 13.8837368760 +57 48 11.400917472   8.05 6.52     M4II 47 1
5 HD 12392 Pe* 02 01 22.7646545736 -04 48 11.814028272   9.56 8.48     G8II 25 0
6 HD 16458 SB* 02 47 47.7257592048 +81 26 54.505744152   7.091 5.781     K1Ba5 169 0
7 * rho02 Ari LP* 02 55 48.4979998 +18 19 53.902936 8.56 7.44 5.93 3.51 1.34 M6-III: 232 0
8 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
9 * rho Per LP* 03 05 10.59385 +38 50 24.9943 6.83 5.04 3.39 1.59 -0.03 M4+IIIa 330 0
10 V* BD Cam Sy* 03 42 09.3255143544 +63 13 00.468590376 8.56 6.74 5.11 3.49 2.11 S3.5/2 220 0
11 HD 27271 SB* 04 18 33.8242867776 +02 28 13.904303880   8.53 7.52     G8II 62 0
12 HD 28159 * 04 26 27.1329980496 -00 30 40.295288988   8.83 7.16     K5III 25 0
13 HD 31487 SB* 04 59 03.7278166656 +51 56 32.031317148   9.47 8.12     G8IIIBa3 62 0
14 V* V1261 Ori Sy* 05 22 18.6449207496 -08 39 58.031922816 10.28 8.57 6.77     S4,1 170 0
15 HD 43389 SB* 06 15 47.0680552296 -02 23 08.240872344 11.26 9.80 8.32     K0/1IIICNIIp 56 1
16 * mu. Gem LP* 06 22 57.62686 +22 30 48.8979 6.37 4.51 2.87 1.30 -0.08 M3IIIab 392 1
17 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
18 V* V613 Mon S* 06 48 22.2962629896 +05 32 30.062068944   9.53 7.78     S3/2 89 0
19 V* KR CMa S* 06 48 50.5905123984 -20 25 32.256147180   9.97 8.50     M4S 43 0
20 HD 50082 SB* 06 51 53.9588741976 +06 36 24.481624140   8.46 7.42     K0_Ba3 63 1
21 CPD-19 1672 S* 07 03 12.0278724912 -19 47 45.918711780   11.52 9.81     S3*3 11 0
22 V* AA Cam S* 07 14 52.0696706376 +68 48 15.359511204   9.23 7.79     M5S 77 0
23 HD 60197 SB* 07 32 07.9568347800 -29 38 06.460881684 11.52 9.50 7.76     K3.5III:Ba3.5 64 0
24 V* NQ Pup S* 07 53 05.2704648648 -11 37 29.352872136   9.34 7.64     S4.5/2 100 0
25 CSS 454 S* 08 04 40.8861230688 -03 04 25.762616760   12.39 10.39     S 16 0
26 HD 88562 SB* 10 12 29.9425836816 -15 53 23.272044576   10.06 8.52     K1III 52 0
27 HD 100503 SB* 11 33 47.2427646768 -31 05 16.761505128   10.68 8.73     G/KpBa 51 0
28 HD 116869 Pe* 13 26 37.9601388312 -04 26 44.934115776   10.47 9.50     G8III:Fe-0.5CH1Ba1 37 0
29 HD 119667 S* 13 44 45.1396113792 -03 32 00.234827304   10.10 8.42     M0III 48 0
30 HD 120620 SB* 13 50 41.6578375656 -04 16 04.875004200   10.78 9.60     K0(III) 33 0
31 HD 121447 SB* 13 55 46.9655016048 -18 14 56.486226336 11.50 9.61 7.80     C2,1_CH4:_Ba4 130 0
32 HD 123949 SB* 14 10 59.3114487936 -19 08 38.227483320 11.40 10.10 8.70     K1pBa 55 0
33 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
34 HD 123396 Pe* 14 17 31.5578897304 -83 32 52.136889108   10.14 8.96     G8/K0II/IIIp 46 0
35 V* RR UMi LP* 14 57 35.0095879431 +65 55 56.814643584 7.86 6.19 4.54 2.69 0.97 M4.5III 195 0
36 V* V530 Lyr S* 18 30 34.5709214544 +36 14 56.999721696   9.01 7.44     S3+/1-III: 61 0
37 HD 178717 SB* 19 09 22.0095424584 +10 14 28.239748008   9.05 7.14     K3.5III:Ba4+ 119 0
38 HD 191226 S* 20 07 26.5352829840 +36 34 03.963225900   9.16 7.33     M1-3SIIIa 63 0
39 HD 191589 S* 20 09 32.9862045768 +33 40 53.851811988   8.772 7.244     M0SIb/II 60 0
40 V* AD Cyg S* 20 31 36.5133153840 +32 33 52.355493648   11.22 8.87     S5/5 66 0
41 V* V2141 Cyg S* 20 57 53.1770842392 +44 47 17.342113776   9.13 7.48     MS 65 0
42 HD 199939 SB* 20 58 43.4942605752 +44 24 52.482256560   8.74 7.44     G9III:Ba4 90 0
43 V* HR Peg S* 22 54 35.6272159944 +16 56 30.606025560 9.970 8.160 6.360     S4+/1+ 137 0

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