2015A&A...581A..22A


Query : 2015A&A...581A..22A

2015A&A...581A..22A - Astronomy and Astrophysics, volume 581A, 22-22 (2015/9-1)

Carbon-enhanced metal-poor stars: a window on AGB nucleosynthesis and binary evolution. II. Statistical analysis of a sample of 67 CEMP-s stars.

ABATE C., POLS O.R., IZZARD R.G. and KARAKAS A.I.

Abstract (from CDS):

Many of the carbon-enhanced metal-poor (CEMP) stars that we observe in the Galactic halo are found in binary systems and show enhanced abundances of elements produced by the slow neutron-capture process (s-elements). The origin of the peculiar chemical abundances of these CEMP-s stars is believed to be accretion in the past of enriched material from a primary star in the asymptotic giant branch (AGB) phase of its evolution. We investigate the mechanism of mass transfer and the process of nucleosynthesis in low-metallicity AGB stars by modelling the binary systems in which the observed CEMP-s stars were formed. For this purpose we compare a sample of 67 CEMP-s stars with a grid of binary stars generated by our binary evolution and nucleosynthesis model. We classify our sample CEMP-s stars in three groups based on the observed abundance of europium. In CEMP-s/r stars the europium-to-iron ratio is more than ten times higher than in the Sun, whereas it is lower than this threshold in CEMP-s/nr stars. No measurement of europium is currently available for CEMP-s/ur stars. On average our models reproduce the abundances observed in CEMP-s/nr stars well, whereas in CEMP-s/r stars and CEMP-s/ur stars the abundances of the light-s elements (strontium, yttrium, zirconium) are systematically overpredicted by our models, and in CEMP-s/r stars the abundances of the heavy-s elements (barium, lanthanum) are underestimated. In all stars our modelled abundances of sodium overestimate the observations. This discrepancy is reduced only in models that underestimate the abundances of most of the s-elements. Furthermore, the abundance of lead is underpredicted in most of our model stars, independent of the metallicity. These results point to the limitations of our AGB nucleosynthesis model, particularly in the predictions of the element-to-element ratios. In our models CEMP-s stars are typically formed in wide systems with periods above 10000-days, while most of the observed CEMP-s stars are found in relatively close orbits with periods below 5000-days. This evidence suggests that either the sample of CEMP-s binary stars with known orbital parameters is biased towards short periods or that our wind mass-transfer model requires more efficient accretion in close orbits.

Abstract Copyright:

Journal keyword(s): stars: abundances - stars: AGB and post-AGB - binaries: general - stars: chemically peculiar - stars: Population II - Galaxy: halo

VizieR on-line data: <Available at CDS (J/A+A/581/A22): table1.dat table2.dat table3.dat table4.dat table5.dat table6.dat table7.dat table8.dat>

Simbad objects: 66

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Number of rows : 66
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 HE 0012-1441 Pe* 00 15 27.0563508456 -14 24 37.626125112     16.40     CEMP-s 14 0
3 HE 0024-2523 Pe* 00 27 27.6486469632 -25 06 28.289948508 15.067 15.32 14.91     CEMP-s 68 0
4 BPS CS 31062-0050 Pe* 00 30 31.0646803224 -12 05 10.877225064   13.7 13.05 12.681 12.309 CEMP-r/s 65 0
5 CD-24 266 BS* 00 40 47.9313619824 -24 07 34.183333668   12.955 12.656 12.441 12.216 CEMP-s 94 0
6 SB 960 Pe* 00 44 03.5698629048 -13 55 26.268999384   12.69 12.15 11.806 11.483 CEMP-s 110 0
7 CD-31 306 BS* 00 50 15.7694498016 -30 59 56.192808696   12.73 12.72     F3VkA2mA2 34 0
8 HD 5223 SB* 00 54 13.6098985200 +24 04 01.515842760   9.88 8.47     C-H2IIIb: 121 0
9 CD-26 304 SB* 00 57 18.1374361752 -25 26 09.696130944   13.57 12.69 12.198 11.759 CEMP-s 72 1
10 HE 0131-3953 Pe* 01 33 36.4628527632 -39 37 52.143313800     15.979   15.323 CEMP-s 23 0
11 HE 0143-0441 Pe* 01 45 37.9166141208 -04 26 43.244756916     16.38     CEMP-s 29 0
12 HE 0202-2204 Pe* 02 04 50.0173418688 -21 50 10.473005688     15.375   14.575 ~ 20 0
13 HE 0206-1916 Pe* 02 09 19.6321025088 -19 01 55.451633016   15.133 13.999 13.458 12.987 CEMP-s 21 0
14 V* V Ari LP? 02 15 00.0771848760 +12 14 23.612094312   10.8 9.80     C-H3.5 106 0
15 HE 0212-0557 Pe* 02 15 02.5102061448 -05 43 23.655462024     14.70     CEMP-s 15 0
16 HE 0231-4016 Pe* 02 33 44.3982295296 -40 03 42.729581232   16.494 16.090 15.788 15.475 CEMP-s 20 0
17 HE 0322-1504 Pe* 03 24 40.1041658856 -14 54 24.352834140   15.809 14.294 13.133 12.556 CEMP-s 13 0
18 BPS CS 29526-0110 Pe* 03 27 43.6392396600 -23 00 29.924362260   13.71 13.35 13.116 12.834 CEMP-r/s 51 0
19 HE 0338-3945 Pe* 03 39 55.0068570984 -39 35 42.902896452   15.753 15.333 15.098 14.787 CEMP-r/s 36 0
20 HE 0430-4404 Pe* 04 31 38.1101576880 -43 57 48.707311788     15.724   15.166 CEMP-s 18 0
21 HE 0441-0652 Pe* 04 43 29.8848378360 -06 46 53.520042180   15.250 14.228 13.678 13.106 CEMP-s 15 0
22 HE 0507-1430 Pe* 05 10 07.6176113760 -14 26 31.742234844   16.06 14.40 13.693 13.104 CEMP-s 10 0
23 HE 0534-4548 Pe* 05 36 06.2090207928 -45 46 55.872922656   15.23 13.80 13.14 12.515 CEMP-s 7 0
24 SDSS J091243.72+021623.6 Pe* 09 12 43.7229065184 +02 16 23.716384212           CEMP-s 23 0
25 2MASS J09240185+4059288 Pe* 09 24 01.8543037368 +40 59 28.798863468           CEMP-s 18 0
26 HE 1045-1434 Pe* 10 47 44.1846861936 -14 50 22.527341736   15.83 14.60 14.036 13.6 C 7 0
27 HE 1105+0027 Pe* 11 07 49.5058798584 +00 11 38.346763524   16.038 15.646 15.358 15.018 CEMP-s 27 0
28 BD+04 2466 Pe* 11 26 49.1891119944 +03 51 51.641714700   11.22 10.67 10.45   KIIvw 81 0
29 HE 1135+0139 Pe* 11 38 09.8529236352 +01 22 44.044584024   16.322 15.829 15.484 15.084 CEMP-s 19 0
30 HE 1157-0518 Pe* 12 00 18.0605588424 -05 34 43.117716900   16.273 15.120 14.635 14.128 CEMP-s 12 0
31 HE 1305+0007 Pe* 13 08 03.8464604328 -00 08 47.502965400   13.98 12.223 11.541 11.071 CEMP-s 30 0
32 2MASS J13364604+4503086 Pe* 13 36 46.0325838312 +45 03 08.641824120   14.57 13.8 13.401 12.974 CEMP-r/s 17 0
33 HE 1429-0551 Pe* 14 32 31.2973339296 -06 05 00.201354252   14.015 12.606 11.995 11.537 CEMP-s 23 0
34 HE 1430-1123 Pe* 14 33 33.6342616032 -11 37 07.194252324   16.504 16.127 15.787 15.403 CEMP-s 15 0
35 HE 1434-1442 Pe* 14 37 26.5888740672 -14 54 59.398236216     15.40   15.395 CEMP-s 16 0
36 HE 1443+0113 Pe* 14 46 16.3657593360 +01 01 09.894018540     15.74     CEMP-s 12 0
37 HE 1447+0102 Pe* 14 50 15.0435395520 +00 50 15.086778720   15.632 14.614 14.121 13.676 CEMP-s 15 0
38 BPS CS 30301-0015 Pe* 15 08 56.8432075560 +02 30 18.627466716   14.04 13.04   12.063 CEMP-s 45 0
39 HE 1523-1155 Pe* 15 26 41.0446929408 -12 05 42.660193380   14.571 13.225 12.622 12.138 CEMP-s 19 0
40 HE 1528-0409 Pe* 15 30 54.3052338480 -04 19 40.363602024   16.003 14.757 14.159 13.681 CEMP-s 13 0
41 LP 625-44 Pe* 16 43 14.0377103880 -01 55 30.411443424   12.84 11.68     CEMP-s 106 0
42 2MASS J16510881+5712277 Pe* 16 51 08.8035670560 +57 12 27.769041180   14.80 14.4 13.986 13.672 CEMP-s 16 0
43 ATO J256.8913+58.8499 RR* 17 07 33.9318852312 +58 50 59.711493732   16.209 15.635 15.977   F5kA2Bapec 27 0
44 HD 187216 Pe* 19 24 18.3437183760 +85 21 57.189325176   11.2 9.56     C3,3_CH5: 74 2
45 HD 187861 SB* 19 56 26.9442832128 -65 22 08.014212084   10.42 9.18     CEMP-rs 63 0
46 BPS CS 22964-0161 SB* 20 03 25.5363989280 -38 38 35.322004572   14.9 14.41 14.63   CEMP-s 43 0
47 HD 196944 SB* 20 40 46.0815001992 -06 47 50.604476604   9.01 8.40 8.08   CEMP-rs 101 0
48 BPS CS 22880-0074 Pe* 20 46 03.2162534976 -20 59 14.110203840   13.84 13.27 12.770 12.382 CEMP-s 47 0
49 SDSS J204728.84+001553.8 Pe* 20 47 28.8409584360 +00 15 53.867748672           CEMP-s 18 0
50 HD 198269 SB* 20 48 36.7391782248 +17 50 23.718943680   9.41 8.12     C-H3IV: 84 0
51 BPS CS 22898-0027 Pe* 21 05 45.0996805992 -18 36 57.501493128   13.26 12.76 12.476 12.094 CEMP-r/s 83 0
52 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
53 HE 2134-3940 Pe* 21 37 45.7673945880 -39 27 22.313379600   13.790 12.660 12.160 11.760 KIIvw 85 0
54 BPS CS 22956-0028 SB* 21 44 48.7055162280 -63 22 09.736708872   13.317 13.0     CEMP-s 27 0
55 HE 2148-1247 Pe* 21 51 17.9096426016 -12 33 41.557315896   15.2 14.79     CEMP-r/s 47 0
56 HE 2150-0825 Pe* 21 53 00.1626443880 -08 11 18.214399320     14.959   14.316 ~ 14 0
57 HE 2158-0348 Pe* 22 00 39.9762999888 -03 34 12.068228532     15.71   14.726 CEMP-s 22 0
58 BPS CS 22881-0036 Pe* 22 07 58.4409920904 -40 44 16.477523484   14.42 13.95 13.633 13.278 CEMP-s 38 0
59 HE 2221-0453 Pe* 22 24 25.6258778472 -04 38 02.318811828   15.098 13.650 12.942 12.376 CEMP-s 19 0
60 HE 2227-4044 Pe* 22 30 19.0908294672 -40 29 13.060819536   15.445 14.925 14.606 14.280 CEMP-s 16 0
61 HE 2228-0706 Pe* 22 31 24.4714115856 -06 50 51.245788020   14.353 13.332 12.797 12.353 CEMP-s 13 0
62 HE 2232-0603 Pe* 22 34 47.4285458448 -05 48 17.341180596   16.861 16.51 15.894 15.591 ~ 17 0
63 HE 2240-0412 Pe* 22 42 58.0813480512 -03 56 34.097034732   16.318 15.807 15.496 15.168 CEMP-s 16 0
64 HE 2258-6358 Pe* 23 01 48.6559441632 -63 42 25.117355556   15.42 14.30 14.07   CEMP-s 11 0
65 BPS CS 30338-0089 Pe* 23 15 49.9735222104 +10 19 26.170039308   15.107 14.144 13.632 13.176 CEMP-s 16 0
66 BPS CS 22945-0017 Pe* 23 20 55.6277405064 -63 15 36.786796848   14.83 14.44 14.50   ~ 25 0

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