2005ApJ...632..611A


Query : 2005ApJ...632..611A

2005ApJ...632..611A - Astrophys. J., 632, 611-637 (2005/October-2)

Spectroscopic studies of very metal-poor stars with the Subaru high dispersion spectrograph. III. Light neutron-capture elements.

AOKI W., HONDA S., BEERS T.C., KAJINO T., ANDO H., NORRIS J.E., RYAN S.G., IZUMIURA H., SADAKANE K. and TAKADA-HIDAI M.

Abstract (from CDS):

Elemental abundance measurements have been obtained for a sample of 18 very metal-poor stars using spectra obtained with the Subaru Telescope High Dispersion Spectrograph. Seventeen stars, among which 16 are newly analyzed in the present work, were selected from candidate metal-poor stars identified in the HK survey of Beers and colleagues. The metallicity range covered by our sample is -3.1≲[Fe/H]≲-2.4. The abundances of carbon, α-elements, and iron-peak elements determined for these stars confirm the trends found by previous work. One exception is the large overabundance of Mg, Al, and Sc found in BS 16934-002, a giant with [Fe/H]=-2.8. Interestingly, this is the most metal-rich star (by about 1 dex in [Fe/H]) known with such large overabundances in these elements. Furthermore, BS 16934-002 does not share the large overabundances of carbon that are associated with the two other, otherwise similar, extremely metal-poor stars CS 22949-037 and CS 29498-043. By combining our new results with those of previous studies, we investigate the distribution of neutron-capture elements in very metal-poor stars, focusing on the production of the light neutron-capture elements (e.g., Sr, Y, and Zr). Large scatter is found in the abundance ratios between the light and heavy neutron-capture elements (e.g., Sr/Ba, Y/Eu) for stars with low abundances of heavy neutron-capture elements. Most of these stars have extremely low metallicity ([Fe/H]≲-3). By contrast, the observed scatter in these ratios is much smaller in stars with excesses of heavy neutron-capture elements and with higher metallicity. These results can be naturally explained by assuming that two processes independently enriched the neutron-capture elements in the early Galaxy. One process increases both light and heavy neutron-capture elements and affects stars with [Fe/H]≳-3, while the other process contributes only to the light neutron-capture elements and affects most stars with [Fe/H]≳-3.5. Interestingly, the Y/Zr ratio is similar in stars with high and low abundances of heavy neutron-capture elements. These results provide constraints on modeling of neutron-capture processes, in particular, those responsible for the nucleosynthesis of light neutron-capture elements at very low metallicity.

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Journal keyword(s): Nuclear Reactions, Nucleosynthesis, Abundances - Stars: Abundances - Stars: Population II

Simbad objects: 23

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Number of rows : 23
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 SB 960 Pe* 00 44 03.5698629048 -13 55 26.268999384   12.69 12.15 11.806 11.483 CEMP-s 114 0
2 BD-16 251 RG* 01 29 31.1311443552 -16 00 45.495314460 12.527 12.427 11.642 11.189 10.713 CEMP 318 0
3 2MASS J11012043-1338384 Pe* 11 01 20.4200403120 -13 38 38.603857560 14.198 14.14 13.43 12.993 12.518 ~ 6 0
4 2MASS J13055616+2510161 Pe* 13 05 56.1655547064 +25 10 16.025134656   14.42 13.8 13.367 12.943 ~ 7 0
5 2MASS J13262814+2138429 Pe* 13 26 28.1414236104 +21 38 42.851996448   13.26 12.6 12.113 11.657 ~ 12 0
6 BPS BS 16934-0002 Pe* 13 29 46.5066859200 +16 15 45.145424556   13.733 12.819 12.239 11.670 ~ 17 0
7 2MASS J13492196+3544502 Pe* 13 49 21.9625001928 +35 44 50.151861276   14.03 13.3 12.842 12.333 ~ 10 0
8 HD 122563 Pe* 14 02 31.8455084952 +09 41 09.944391876 7.47 7.10 6.19 5.37 4.79 G8:III:Fe-5 920 0
9 BPS BS 16083-0172 Pe* 14 50 41.4358262496 +48 45 13.540748220   13.74 13.13 13.025 12.594 ~ 8 0
10 2MASS J14543927+0421380 Pe* 14 54 39.2685981792 +04 21 38.099145888   13.02 12.32 11.849 11.376 ~ 53 0
11 2MASS J15051979+0617069 Pe* 15 05 19.8064435128 +06 17 06.933083424   13.64 12.88 12.387 11.893 CEMP 22 0
12 BPS CS 30306-0132 Pe* 15 14 18.9191634456 +07 27 02.680959780   13.62 12.73 12.421 11.948 ~ 43 0
13 BPS CS 30312-0059 Pe* 15 34 48.8386814136 -01 23 37.343777064   13.85 13.14 12.596 12.065 ~ 29 0
14 TYC 5030-1015-1 Pe* 15 48 41.8874319000 -06 52 37.316534556   12.74 12.13 11.367 10.817 ~ 6 0
15 BPS BS 16084-0160 Pe* 16 28 50.7923247984 +54 37 06.886218324   13.94 13.12 12.630 12.103 ~ 22 0
16 2MASS J16391853+6057426 Pe* 16 39 18.5345769192 +60 57 42.547552920   13.50 12.79   11.786 ~ 20 0
17 BPS CS 29498-0043 Pe* 21 03 52.1197651440 -29 42 50.344181712   14.8 13.72 13.013 12.406 CEMP-no 100 0
18 2MASS J21193930-2652395 Pe* 21 19 39.3112837872 -26 52 39.678366684   13.59 12.8 12.137 11.720 ~ 5 0
19 HE 2157-3404 Pe* 22 00 17.7010220736 -33 50 03.808011264   13.76 13.13 13.08   ~ 6 0
20 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
21 BPS CS 22886-0042 Pe* 22 20 25.8163819488 -10 23 20.107482000   14.106 13.275 12.763 12.269 ~ 28 0
22 2MASS J22214882+0228448 Pe* 22 21 48.8262598080 +02 28 44.867730936 13.291 13.4 12.74 12.325 12.013 ~ 46 0
23 HE 2323-0256 Pe* 23 26 29.8073738880 -02 39 58.036383180   15.125 14.321 14.289 13.358 CEMP-no 184 0

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