2025A&A...693A.293L


Query : 2025A&A...693A.293L

2025A&A...693A.293L - Astronomy and Astrophysics, volume 693A293 (2025/1-1)

Chemical Evolution of R-process Elements in Stars (CERES) III. Chemical abundances of neutron capture elements from Ba to Eu.

LOMBARDO L., HANSEN C.J., RIZZUTI F., CESCUTTI G., MASHONKINA L.I., FRANCOIS P., BONIFACIO P., CAFFAU E., ALENCASTRO PULS A., FERNANDES DE MELO R., GALLAGHER A.J., SKULADOTTIR A., KOCH-HANSEN A.J. and SBORDONE L.

Abstract (from CDS):

Context. The chemical abundances of elements such as barium and the lanthanides are essential to understand the nucleosynthesis of heavy elements in the early Universe as well as the contribution of different neutron capture processes (for example slow versus rapid) at different epochs.
Aims. The Chemical Evolution of R-process Elements in Stars (CERES) project aims to provide a homogeneous analysis of a sample of metal-poor stars ([Fe/H]←1.5) to improve our understanding of the nucleosynthesis of neutron capture elements, in particular the r-process elements, in the early Galaxy.
Methods. Our data consist of a sample of high resolution and high signal-to-noise ratio UVES spectra. The chemical abundances were derived through spectrum synthesis, using the same model atmospheres and stellar parameters as derived in the first paper of the CERES series.
Results. We measured chemical abundances or upper limits of seven heavy neutron capture elements (Ba, La, Ce, Pr, Nd, Sm, and Eu) for a sample of 52 metal-poor giant stars. We estimated through the mean shift clustering algorithm that at [Ba/H]=-2.4 and [Fe/H]=-2.4 a variation in the trend of [X/Ba], with X=La,Nd,Sm,Eu, versus [Ba/H] occurs. This result suggests that, for [Ba/H]←2.4, Ba nucleosynthesis in the Milky Way halo is primarily due to the r-process, while for [Ba/H]>-2.4 the effect of the s-process contribution begins to be visible. In our sample, stars with [Ba/Eu] compatible with a Solar System pure r-process value (hereafter, r-pure) do not show any particular trend compared to other stars, suggesting r-pure stars may form in similar environments to stars with less pure r-process enrichments.
Conclusions. Homogeneous investigations of high resolution and signal-to-noise ratio spectra are crucial for studying the heavy elements formation, as they provide abundances that can be used to test nucleosynthesis models as well as Galactic chemical evolution models.

Abstract Copyright: © The Authors 2025

Journal keyword(s): nuclear reactions, nucleosynthesis, abundances - stars: abundances - stars: Population II - Galaxy: abundances - Galaxy: stellar content

VizieR on-line data: <Available at CDS (J/A+A/693/A293): stars.dat table1.dat>

Status at CDS : All or part of tables of objects will be ingested in SIMBAD with priority 1.

Simbad objects: 32

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Number of rows : 32
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 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1498 4
2 NAME Tri II G 02 13 17.40 +36 10 42.4           ~ 164 0
3 MCG-06-07-001 G 02 39 59.3 -34 26 57   9.02 7.4     ~ 1894 1
4 NAME Reticulum II G 03 35 42.1 -54 02 57           ~ 375 0
5 BD-13 899 PM* 04 30 51.4238564448 -13 34 08.141118600   10.75 10.18     ~ 6 0
6 TYC 5922-517-1 Pe* 05 47 20.8069100832 -17 39 40.994450640   13.42 11.92     ~ 9 0
7 TYC 4840-159-1 Pe* 07 47 15.8241428904 -04 05 46.145440464   12.18 10.55     ~ 6 0
8 NAME UMa II Galaxy G 08 51 30.0 +63 07 48     13.3     ~ 410 0
9 TYC 8931-1111-1 Pe* 09 00 52.5868989960 -62 22 52.848219072   12.645 11.340     ~ 13 0
10 TYC 8939-2532-1 Pe* 09 08 07.5084957024 -66 07 33.896463024   12.50 11.50     ~ 9 0
11 TYC 9200-2292-1 Pe* 09 19 16.2942147144 -69 58 39.857086488   12.66 11.38     ~ 9 0
12 NAME Segue 1 G 10 07 03.2 +16 04 25     15.3     ~ 517 1
13 NAME Sextans dSph LSB 10 13 02.9 -01 36 53   12 10.4     ~ 921 0
14 HD 88609 Pe* 10 14 28.9853799600 +53 33 39.342740796 9.930 9.540 8.620 7.78 7.15 G5IIIw 217 0
15 NAME Leo IV LSB 11 32 57.0 -00 32 00     15.1     ~ 419 1
16 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 50 0
17 NAME Coma Dwarf Galaxy G 12 26 59.0 +23 54 15     14.1     ~ 482 1
18 BPS BS 16085-0050 Pe* 12 37 46.6781374776 +19 22 49.551755664 12.965 12.93 12.16 11.668 11.186 ~ 32 0
19 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
20 NAME CVn I dSph G 13 28 03.5 +33 33 21     13.1     ~ 352 1
21 NAME Bootes Dwarf Spheroidal Galaxy G 14 00 00.0 +14 30 00     12.8     ~ 491 0
22 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
23 TYC 9427-1414-1 Pe* 14 13 11.1788763744 -76 09 50.443206336   11.56 10.56     ~ 7 0
24 Z 318-18 G 15 09 08.0 +67 13 21   13.60 10.6     ~ 1459 0
25 NAME Hercules Dwarf Galaxy G 16 31 02.0 +12 47 30     14.0     ~ 379 1
26 Z 300-12 G 17 20 14.335 +57 55 16.39   12.40 10.6     ~ 1428 1
27 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2438 2
28 TYC 8444-76-1 * 22 13 20.4894810480 -51 37 38.689403592   12.223 11.630     ~ 15 0
29 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
30 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 43 0
31 HE 2252-4225 Pe* 22 54 58.5673558608 -42 09 19.386504792     14.878   13.855 ~ 30 0
32 HE 2327-5642 Pe* 23 30 37.0896973176 -56 26 14.385030648   14.590 13.881 13.425 12.948 ~ 51 0

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