2025A&A...695A..94W


Query : 2025A&A...695A..94W

2025A&A...695A..94W - Astronomy and Astrophysics, volume 695A94 (2025/3-1)

Barium and europium abundances in high- and low-α halo stars.

WANG G., LI J., CHANG Z., SHI J., LI Z., TIAN M. and CUI W.

Abstract (from CDS):

Context. Prior studies have found that there are two distinct halo populations with a clear separation in [α/Fe], known as the high-α and low-α populations. Certain other elements, such as [C/Fe], [O/Fe], and [Na/Fe], as well as [Cu/Fe], also show a clear distinction between the high- and low-α halo populations. However, the abundance ratios, such as [Li/Fe] and [Mn/Fe], are indistinguishable between these two halo populations.
Aims. This work is aim at determining the abundances of barium and europium for a sample of halo stars, including 29 high-α and 19 low-α halo stars, and to investigate the distributions of [Ba/Fe] and [Eu/Fe]. We also present the fraction of barium isotopes with an odd mass number (fodd) in the sample stars to estimate the relative contribution of the r- and s-processes to the abundance of Ba.
Methods. The abundance ratios of [Ba/Fe] and [Eu/Fe] were determined by the spectral synthesis method based on the high-resolution and high signal-to-noise ratio (S/N) spectra collected from the ESO/ST-ECF Science Archive of VLT/UVES and NOT/FIES spectrographs. Non-local thermodynamic equilibrium (NLTE) effects were also considered. The fodd value was estimated by fitting the profile of the Ba II resonance line at λ4554 Å.
Results. The NLTE effect is needed to be included to fully capture the line profiles for both Ba II and Eu II, however, the NLTE corrections for the barium and europium are different. For Ba, the NLTE corrections are negative compared to the results of thermodynamic equilibrium, except the star with lowest metallicity, and they become smaller with decreasing of [Fe/H]. For Eu, the NLTE corrections are positive and independent of stellar metallicity. It is found that both the abundances of [Ba/Fe] and [Eu/Fe] in the high-and low-α halo stars are mixed together. Although the [Eu/Ba] ratios cannot be distinguished clearly between the high- and low-α halo populations, stars with [Eu/Ba] ≥ 0.7 dex can only be found in the low-α population. Similar to [Eu/Ba], the ratios of fodd cannot be separated among the high- and low-α halo populations, although the stars with the highest fodd (≥0.4) can only be seen in the low-α stars with [Eu/Ba] ≥ 0.7 dex.
Conclusions. Our results indicate that both the [Ba/Fe] and [Eu/Fe] ratios are indistinguishable among the high- and low-α halo stars, while [Eu/Mg] is able to separate the two halo populations well. Combining the highest [Eu/Ba] and fodd ratios, as well as the lower [α/Fe] in some low-α halo stars, we can infer that the r-process is dominating in these low-α halo stars and they are likely to have been accreted from dwarf galaxies as proposed by previous studies.

Abstract Copyright: © The Authors 2025

Journal keyword(s): line: formation - line: profiles - stars: abundances - Galaxy: halo

Simbad objects: 50

goto Full paper

goto View the references in ADS

Number of rows : 50
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 BD-03 56 PM* 00 29 26.6605338732 -02 20 57.055990746   11.269 10.648 10.630   ~ 43 0
2 BD+47 451 SB* 01 34 22.6964788822 +48 44 27.436010103       10.4   M3V 45 0
3 BD+26 377 PM* 02 16 56.5527833760 +27 24 48.417934572   11.06   9.9   G0 40 0
4 BD+32 467 PM* 02 34 13.2132669745 +33 00 05.091152673   11.13   10.2   G0 36 0
5 G 75-31 PM* 02 38 21.5033134703 +02 26 44.370557521   10.968 10.424 10.389   sd?F8 70 0
6 HD 25079 * 03 59 27.2575323960 +11 46 30.460453392   9.87 9.40     F2 9 0
7 HD 276029 PM* 04 03 55.2569638894 +39 44 19.199783595   11.27   10.3   F8 43 0
8 HD 283807 PM* 04 44 42.0610259088 +25 56 09.599948808   10.78   9.7   G0 61 0
9 HD 277559 PM* 05 05 28.7086497622 +40 15 26.368031686   10.08   9.4   F5 65 0
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
11 HD 246067 PM* 05 39 27.4342825426 +03 57 02.683945678       9.9   G0 62 0
12 BD+33 1279a PM* 06 13 49.8286755927 +33 25 02.118887862   11.65   11.1   F8 40 0
13 G 103-69 PM* 06 54 56.2977228912 +35 30 58.636262340   11.55   11.1   sdF2 42 0
14 HD 237822 PM* 09 36 49.5206880772 +57 54 41.015334894   10.59   9.6   G3V 57 0
15 BD+29 1925 SB* 09 38 50.6066348979 +28 24 08.612287954   11.095 10.548 10.448   G5 40 0
16 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
17 G 56-30 PM* 11 21 35.1061968969 +18 11 44.559215421   11.50   10.7   sd?G0 40 0
18 BD+20 2594 PM* 11 23 16.2307856395 +19 53 37.663112839   10.51   9.6   F9 85 0
19 BD+11 2369 PM* 11 32 34.1257455852 +10 54 11.307005592   10.73   9.7   G0 43 0
20 BD+51 1696 Pe* 11 46 35.1556060454 +50 52 54.680145444 10.32 10.47   9.5   sdG0 172 0
21 HD 108177 PM* 12 25 34.9568267745 +01 17 02.259553591 9.87 10.09 9.66 9.21 8.89 F0V 266 0
22 BD+02 2541 PM* 12 26 59.8614892629 +01 33 58.401336422   11.23   9.9   G3 61 0
23 HD 110621 PM* 12 43 43.2215753256 -44 40 31.562765508   10.34 9.92     Fpw 82 0
24 HD 113679 PM* 13 05 52.8245053407 -38 30 59.990193435   10.342 9.797     G2/3V 114 0
25 G 63-26 Pe* 13 24 30.5997776592 +20 27 22.094791164   12.62 12.18 12.5   sd:F 70 0
26 G 150-40 PM* 13 48 52.1482901497 +27 40 09.478619610       10.5   sdF9 45 0
27 HD 132475 PM* 14 59 49.7651173448 -22 00 45.815162806 8.98 9.11 8.55     F5/6V 256 1
28 G 15-23 SB* 15 29 31.6798974496 +06 08 49.881802340   11.67   10.6   ~ 59 0
29 BD+42 2667 Pe* 16 03 13.2988107325 +42 14 46.651500150   10.33   9.6   F5 159 0
30 HD 146296 PM* 16 21 11.3151618845 -71 17 13.024312315   10.37 9.77     G3V 54 0
31 HD 148816 PM* 16 30 28.4586254384 +04 10 41.602836534 7.75 7.81 7.28 6.82 6.49 F7V 329 0
32 HD 159482 PM* 17 34 43.0816088882 +06 00 51.815208744   8.94 8.36     G0V 171 0
33 BD+18 3423 PM* 17 38 15.6094693200 +18 33 25.483804164 10.17 10.27   9.4   F6V 136 0
34 HD 160693 PM* 17 39 36.8721883235 +37 11 01.504256846 8.94 8.92   8.0   G0 224 0
35 HD 160617 Pe* 17 42 49.3234249010 -40 19 15.503834657   9.18 8.7 8.394 8.065 G0 220 0
36 BD-08 4501 PM* 17 47 27.9712915686 -08 46 47.733112329   11.18 10.59     sdF8 140 0
37 HD 163810 ** 17 58 38.4538029750 -13 05 49.654844460 10.15 10.23 9.63     G3V 158 0
38 HD 230409 PM* 19 00 43.3339876251 +19 04 28.418294811   10.78   9.6   G0 97 0
39 HD 177095 PM* 19 03 56.7108988306 -20 27 36.566397661   10.27 9.64     G6V 56 0
40 HD 179626 PM* 19 13 20.7189797919 -00 35 42.325251766   9.701 9.187 8.844 8.489 F5V 136 0
41 G 24-3 Pe* 20 05 44.3170407024 +04 02 52.812418452   10.92   10.2   sdF8 104 0
42 BD+05 4481 PM* 20 20 24.5608644037 +06 01 52.826286539   10.75   10.8   G4 72 0
43 HD 193901 PM* 20 23 35.8471605389 -21 22 14.226959304 9.08 9.22 8.67 8.17 7.87 F7V 298 0
44 HD 194598 PM* 20 26 11.9183775668 +09 27 00.429558608 8.62 8.82 8.34 7.90 7.56 F8 315 0
45 HD 335471 PM* 21 03 06.1287954464 +29 28 56.213243727       9.7   G5 50 0
46 G 232-18 PM* 21 30 37.2926670600 +48 51 59.666714316       10.2   sd?G2 35 0
47 BD+26 4251 PM* 21 43 57.1238515464 +27 23 23.989925868       9.9   F6 100 0
48 BD+07 4841 PM* 22 18 36.5059714907 +08 26 44.962089682   10.84   10.1   G0 127 0
49 G 127-26 PM* 22 23 49.0859208600 +24 23 33.136159236       10.2   F9 45 0
50 NAME Gaia Enceladus-Sausage St* ~ ~           ~ 860 0

To bookmark this query, right click on this link: simbad:objects in 2025A&A...695A..94W and select 'bookmark this link' or equivalent in the popup menu