2014ApJ...797..123H


Query : 2014ApJ...797..123H

2014ApJ...797..123H - Astrophys. J., 797, 123 (2014/December-3)

How many nucleosynthesis processes exist at low metallicity?

HANSEN C.J., MONTES F. and ARCONES A.

Abstract (from CDS):

Abundances of low-metallicity stars offer a unique opportunity to understand the contribution and conditions of the different processes that synthesize heavy elements. Many old, metal-poor stars show a robust abundance pattern for elements heavier than Ba, and a less robust pattern between Sr and Ag. Here we probe if two nucleosynthesis processes are sufficient to explain the stellar abundances at low metallicity, and we carry out a site independent approach to separate the contribution from these two processes or components to the total observationally derived abundances. Our approach provides a method to determine the contribution of each process to the production of elements such as Sr, Zr, Ba, and Eu. We explore the observed star-to-star abundance scatter as a function of metallicity that each process leads to. Moreover, we use the deduced abundance pattern of one of the nucleosynthesis components to constrain the astrophysical conditions of neutrino-driven winds from core-collapse supernovae.

Abstract Copyright: ∼

Journal keyword(s): Galaxy: evolution - Galaxy: stellar content - nuclear reactions, nucleosynthesis, abundances - stars: abundances - supernovae: general

Simbad objects: 18

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Number of rows : 18
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 4306 SB* 00 45 27.1616035344 -09 32 39.785396712 9.80 9.75 9.02 8.75   G3/5w(A) 168 0
2 HD 6268 Pe* 01 03 18.1716378504 -27 52 49.953768852   9.725 9.046 8.601   F/Gw 166 0
3 HE 0104-5300 Pe* 01 06 51.9165053832 -52 44 10.577875704   14.382 13.550 13.038 12.518 CEMP-no 18 0
4 BPS CS 29518-0051 Pe* 01 24 10.0049733024 -28 15 21.115362312 13.567 13.62 13.02 12.594 12.162 ~ 35 0
5 HE 0239-1340 Pe* 02 41 42.3721546152 -13 28 10.603797240   14.73 13.97 13.566 13.080 CEMP-no 64 0
6 BD+42 621 * 02 45 32.4541690680 +42 43 28.889531940   10.60 10.38     A2 13 0
7 HE 0340-5355 Pe* 03 41 34.5669703344 -53 46 18.053151492   16.027 15.249 14.768 14.278 ~ 6 0
8 HE 0409-1212 Pe* 04 12 13.8814287960 -12 05 05.075250072   13.843 12.897   11.764 ~ 72 0
9 HD 88609 Pe* 10 14 28.9853799600 +53 33 39.342740796 9.930 9.540 8.620 7.78 7.15 G5IIIw 217 0
10 2MASS J10151018+4253173 Pe* 10 15 10.1903157288 +42 53 17.362408452   14.19 13.42 12.950 12.470 ~ 19 0
11 HE 1252-0117 Pe* 12 54 59.8421380392 -01 33 35.018228520     14.101   13.124 ~ 6 0
12 2MASS J13492196+3544502 Pe* 13 49 21.9625001928 +35 44 50.151861276   14.03 13.3 12.842 12.333 ~ 10 0
13 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
14 2MASS J14543927+0421380 Pe* 14 54 39.2685981792 +04 21 38.099145888   13.02 12.32 11.849 11.376 ~ 53 0
15 BPS CS 30322-0023 Pe* 21 30 32.1818994960 -46 16 24.614480388   13.447 12.167 11.902 10.908 CEMP-s 59 0
16 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
17 HE 2219-0713 Pe* 22 22 15.7725558672 -06 58 34.483425996     14.212   13.019 ~ 6 0
18 BPS CS 22783-0055 * ~ ~           ~ 2 0

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