2016ApJ...833..181C


Query : 2016ApJ...833..181C

2016ApJ...833..181C - Astrophys. J., 833, 181-181 (2016/December-3)

Constraints of the physics of low-mass AGB stars from CH and CEMP stars.

CRISTALLO S., KARINKUZHI D., GOSWAMI A., PIERSANTI L. and GOBRECHT D.

Abstract (from CDS):

We analyze a set of published elemental abundances from a sample of CH stars which are based on high resolution spectral analysis of ELODIE and SUBARU/HDS spectra. All the elemental abundances were derived from local thermodynamic equilibrium analysis using model atmospheres, and thus they represent the largest homogeneous abundance data available for CH stars to date. For this reason, we can use the set to constrain the physics and the nucleosynthesis occurring in low mass asymptotic giant branch (AGB) s.tars. CH stars have been polluted in the past from an already extinct AGB companion and thus show s-process enriched surfaces. We discuss the effects induced on the surface AGB s-process distributions by different prescriptions for convection and rotation. Our reference theoretical FRUITY set fits only part of the observations. Moreover, the s-process observational spread for a fixed metallicity cannot be reproduced. At [Fe/H] > -1, a good fit is found when rotation and a different treatment of the inner border of the convective envelope are simultaneously taken into account. In order to increase the statistics at low metallicities, we include in our analysis a selected number of CEMP stars and, therefore, we compute additional AGB models down to [Fe/H] = -2.85. Our theoretical models are unable to attain the large [hs/ls] ratios characterizing the surfaces of those objects. We speculate on the reasons for such a discrepancy, discussing the possibility that the observed distribution is a result of a proton mixing episode leading to a very high neutron density (the so-called i-process).

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): nuclear reactions, nucleosynthesis, abundances - physical data and processes - stars: chemically peculiar - stars: evolution - stars: low-mass - stars: low-mass

Simbad objects: 30

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Number of rows : 30
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 224959 SB* 00 02 08.0214788256 -02 49 12.232785144   10.6 9.6     CEMP-rs 96 0
2 HD 26 SB* 00 05 22.2071891760 +08 47 16.095353028 9.80 9.29 8.25 7.49 7.03 C-H1.5 172 0
3 HD 4395 Pe* 00 46 13.7497935576 -11 27 08.552414592   8.39 7.68 7.33   G5/6III 79 0
4 HD 5223 SB* 00 54 13.6098985200 +24 04 01.515842760   9.88 8.47     C-H2IIIb: 121 0
5 * ups02 Cas Pe* 00 56 39.9051464088 +59 10 51.805287084   5.581 4.622     G8.5IIIbFe-0.5 220 0
6 HD 16458 SB* 02 47 47.7257592048 +81 26 54.505744152   7.091 5.781     K1Ba5 162 0
7 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7066 0
8 HD 48565 SB* 06 44 54.9126657408 +20 51 38.338708500   7.746 7.183     hF8gF8mF3 72 0
9 HD 55496 Pe* 07 12 11.3776089792 -22 59 00.613074804   9.30 8.40     CEMP-s 72 1
10 HD 81192 RG* 09 24 45.3356450736 +19 47 11.867336592 8.06 7.50 6.56     G8IIICH 123 0
11 HD 89668 PM* 10 20 43.4054690292 -01 28 11.378535774   10.50 9.41     K3/4V 84 0
12 HD 92545 Pe* 10 40 57.7070010192 -12 11 44.225491848   9.07 9.149 8.25 9.047 F7IV 50 0
13 HE 1152-0355 Pe* 11 55 06.0576787728 -04 12 24.591877812 15.432 13.889 11.43 10.64 10.236 CEMP-s 25 0
14 * omi Vir SB* 12 05 12.5318326945 +08 43 58.866875781 5.75 5.11 4.12 3.38 2.89 G8IIICN0.5CH1Ba1 286 0
15 HD 107574 SB* 12 21 51.8609784600 -18 24 00.253490832   8.99 8.54     F3IV/V 52 0
16 HD 111721 RG* 12 51 25.1948519215 -13 29 28.166947989   8.78 7.97     G6V 163 0
17 HE 1305+0007 Pe* 13 08 03.8464604328 -00 08 47.502965400   13.98 12.223 11.541 11.071 CEMP-s 30 0
18 HD 122202 SB* 14 00 18.9650138088 +04 51 25.109582904   9.85 9.36     F8 20 0
19 HD 125079 Pe* 14 17 20.7180441696 -04 15 57.812210640   9.54 8.63     G2IIIBa1 37 0
20 HD 126681 PM* 14 27 24.9094012952 -18 24 40.454425566   9.939 9.535     G3V 189 0
21 * s Her RG* 16 30 33.5484796848 +20 28 45.074511516   6.484 5.243     G8.5IIICN-2CH-1Fe-1 141 0
22 HD 164922 PM* 18 02 30.8623420470 +26 18 46.805024012   7.79   6.5   G9V 215 1
23 HD 167768 PM* 18 16 53.1010153824 -03 00 26.647248600   6.89 6.00     G8III 97 0
24 HD 188650 Pe* 19 54 48.2511091584 +36 59 44.434621176   6.549 5.781     G1Ib-IICH2Fe-1 74 0
25 HD 198269 SB* 20 48 36.7391782248 +17 50 23.718943680   9.41 8.12     C-H3IV: 84 0
26 HD 201626 SB* 21 09 59.2755833184 +26 36 55.001033532 9.73 9.26 8.16 7.34 6.82 C-H2IV: 155 0
27 HD 204613 SB* 21 27 42.9670649688 +57 19 18.928743348       7.8   G1IIIa:_CH1.5 107 0
28 HD 209621 SB* 22 04 25.1430497160 +21 03 08.991263304   10.41 8.86     C-H3III: 106 0
29 HD 214714 Pe* 22 39 34.3331070264 +37 35 34.141321428   6.875 6.023     G3Ib-II:CN-1CH2Fe-1 67 0
30 HD 216219 SB* 22 50 52.1530053936 +18 00 07.703208072   8.06 7.44     G1II-III:Fe-1CH0.5 119 0

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