2007A&A...462..851B


Query : 2007A&A...462..851B

2007A&A...462..851B - Astronomy and Astrophysics, volume 462851-864 (2007/2-2)

First stars. VII - Lithium in extremely metal poor dwarfs.

BONIFACIO P., MOLARO P., SIVARANI T., CAYREL R., SPITE M., SPITE F., PLEZ B., ANDERSEN J., BARBUY B., BEERS T.C., DEPAGNE E., HILL V., FRANCOIS P., NORDSTROEM B. and PRIMAS F.

Abstract (from CDS):

The primordial lithium abundance is a key prediction of models of big bang nucleosynthesis, and its abundance in metal-poor dwarfs (the Spite plateau) is an important, independent observational constraint on such models. This study aims to determine the level and constancy of the Spite plateau as definitively as possible from homogeneous high-quality VLT-UVES spectra of 19 of the most metal-poor dwarf stars known. Our high-resolution (R∼43000), high S/N spectra are analysed with OSMARCS 1D LTE model atmospheres and turbospectrum synthetic spectra to determine effective temperatures, surface gravities, and metallicities, as well as Li abundances for our stars. Eliminating a cool subgiant and a spectroscopic binary, we find 8 stars to have -3.5<[Fe/H]←3.0 and 9 stars with -3.0<[Fe/H]←2.5. Our best value for the mean level of the plateau is A(Li)=2.10±0.09. The scatter around the mean is entirely explained by our estimate of the observational error and does not allow for any intrinsic scatter in the Li abundances. In addition, we conclude that a systematic error of the order of 200K in any of the current temperature scales remains possible. The iron excitation equilibria in our stars support our adopted temperature scale, which is based on a fit to wings of the Hα line, and disfavour hotter scales, which would lead to a higher Li abundance, but fail to achieve excitation equilibrium for iron. We confirm the previously noted discrepancy between the Li abundance measured in extremely metal-poor turnoff stars and the primordial Li abundance predicted by standard Big-Bang nucleosynthesis models adopting the baryonic density inferred from WMAP. We discuss recent work explaining the discrepancy in terms of diffusion and find that uncertain temperature scales remain a major question.

Abstract Copyright: ∼

Journal keyword(s): nuclear reactions, nucleosynthesis, abundances - Galaxy: halo - Galaxy: abundances - cosmology: observations - stars: Population II

CDS comments: Fig.A1 BS 16023-043 is a probable misprint for BPS BS 16023-0046.

Simbad objects: 35

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Number of rows : 35
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 2MASS J00203619+2347376 Pe* 00 20 36.1923434544 +23 47 37.617775440   14.84 14.5     ~ 28 0
2 BPS CS 29527-0015 Pe* 00 29 10.6814565504 -19 10 07.305102624   14.61 14.24     CEMP-no 59 0
3 HE 0027-3613 Pe* 00 30 15.9610744584 -35 56 51.229784760     14.74     ~ 32 0
4 BPS CS 29518-0020 * 01 12 13.2160928832 -31 00 05.358952296 14.164 14.41 14.00     ~ 20 0
5 2MASS J01183829-3041026 Pe* 01 18 38.3021768400 -30 41 02.851310832 14.730 14.94 14.6     ~ 27 0
6 BPS CS 22953-0037 Pe* 01 25 06.6508649808 -59 16 00.742176912   14.01 13.64   13.13 CEMP-no 45 0
7 BD-10 388 Pe* 01 50 32.6462570064 -09 21 02.840259744   10.78 10.4     F3 102 0
8 BPS CS 31061-0032 Pe* 02 38 43.3009378608 +03 19 02.563623012   14.30 13.90 13.581 13.290 ~ 27 0
9 LP 831-70 PM* 03 06 05.4386096664 -22 19 17.828964660   12.043 11.608 11.598   ~ 52 0
10 CD-33 1173 Pe* 03 19 35.3159594880 -32 50 43.157572008   11.272 10.902 10.421 10.152 CEMP 63 0
11 BPS CS 22177-0009 Pe* 04 07 40.6490981040 -25 02 43.970266068   14.67 14.27     ~ 36 0
12 HD 84937 Pe* 09 48 56.0992891997 +13 44 39.326709913 8.49 8.68 8.32 7.97 7.70 F8Vm-5 831 0
13 BD-13 3442 Pe* 11 46 50.6525751264 -14 06 43.458063768   10.662 10.274     CEMP 117 0
14 2MASS J12482275+2056440 Pe* 12 48 22.7519584056 +20 56 44.029766004   13.88 13.4 13.115 12.706 ~ 25 0
15 HE 1327-2326 Pe* 13 30 05.9394958608 -23 41 49.699340844 13.761 14.01 13.55 13.50 12.803 CEMP-no 258 0
16 Wolf 1492 Pe* 13 40 02.4921849768 -00 02 18.750053436 11.601 11.832 11.451 11.184 10.892 sdF0: 299 0
17 BPS BS 16467-0062 Pe* 13 42 00.6326009568 +17 48 40.826539260   14.69 14.09 13.665 13.216 ~ 53 0
18 HE 1353-2735 SB* 13 56 42.5278858896 -27 49 54.137205768   15.08 14.7     ~ 10 0
19 2MASS J14005447+2246423 Pe* 14 00 54.4740571128 +22 46 42.087313956 14.317 14.548 14.2     ~ 26 0
20 Ross 841 Pe* 14 02 30.0900761861 -05 39 05.181979951   11.508 11.149 10.866 10.576 sdA3 161 0
21 BPS BS 16968-0061 Pe* 15 01 06.1171458744 +03 42 45.573411168   13.73 13.22 13.39   ~ 36 0
22 UCAC2 31517587 Pe* 15 08 29.6579865432 -00 35 59.273507796   13.37 12.95   12.37 ~ 27 0
23 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 985 0
24 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 2103 0
25 HD 338529 PM* 19 32 31.9104668184 +26 23 26.117367216   9.72   9.2   B5 213 0
26 UCAC2 7177623 Pe* 19 42 26.8926894816 -56 58 34.059037980   14.27 13.63     ~ 57 0
27 LP 815-43 Pe* 20 38 13.2998605176 -20 26 10.850795808   11.31 10.72     ~ 82 0
28 BPS CS 29506-0007 Pe* 21 20 28.6541822328 -20 46 22.955304144     14.18     ~ 32 0
29 BPS CS 29506-0090 Pe* 21 30 28.8706762776 -22 10 41.578379040     14.33     ~ 29 0
30 BPS CS 22948-0093 Pe* 21 50 31.5180047928 -41 07 49.355148468   15.54 15.18     ~ 37 0
31 BPS CS 22965-0054 Pe* 22 06 30.2933030688 -02 32 34.433318220   15.69 15.07 14.732 14.072 CEMP-no 39 0
32 CD-24 17504 Pe* 23 07 20.2534619736 -23 52 35.954286096   12.51 12.18     CEMP-no 94 0
33 BPS CS 22888-0031 Pe* 23 11 32.4788498208 -35 26 42.872735796   15.31 14.90     CEMP-no 39 0
34 2MASS J23350705-3022543 Pe* 23 35 07.0484945928 -30 22 54.278132700 14.694 14.97 14.6     ~ 32 0
35 SB 966 Pe* 23 53 40.2978963936 -26 58 43.988391156   13.50 13.050     sdF/G? 38 0

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