2022A&A...665A..10L


Query : 2022A&A...665A..10L

2022A&A...665A..10L - Astronomy and Astrophysics, volume 665A, 10-10 (2022/9-1)

Chemical Evolution of R-process Elements in Stars (CERES). I. Stellar parameters and chemical abundances from Na to Zr.

LOMBARDO L., BONIFACIO P., FRANCOIS P., HANSEN C.J., CAFFAU E., HANKE M., SKULADOTTIR A., ARCONES A., EICHLER M., REICHERT M., PSALTIS A., KOCH HANSEN A.J. and SBORDONE L.

Abstract (from CDS):


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). We present the stellar parameters and the chemical abundances of elements up to Zr for a sample of 52 giant stars.
Methods. We relied on a sample of high signal-to-noise UVES spectra. We determined stellar parameters from Gaia photometry and parallaxes. Chemical abundances were derived using spectrum synthesis and model atmospheres.
Results. We determined chemical abundances of 26 species of 18 elements: Na, Mg, Al, Si, Ca, Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Sr, Y, and Zr. For several stars, we were able to measure both neutral and ionised species, including Si, Sc, Mn, and Zr. We have roughly doubled the number of measurements of Cu for stars at [Fe/H] ≤ -2.5. The homogeneity of the sample made it possible to highlight the presence of two Zn-rich stars ([Zn/Fe] ∼ +0.7), one r-rich and the other r-poor. We report the existence of two branches in the [Zn/Fe] versus [Ni/Fe] plane and suggest that the high [Zn/Fe] branch is the result of hypernova nucleosynthesis. We discovered two stars with peculiar light neutron-capture abundance patterns: CES1237+1922 (also known as BS 16085-0050), which is ∼1 dex underabundant in Sr, Y, and Zr with respect to the other stars in the sample, and CES2250-4057 (also known as HE 2247-4113), which shows a ∼1 dex overabundance of Sr with respect to Y and Zr.
Conclusions. The high quality of our dataset allowed us to measure hardly detectable ions. This can provide guidance in the development of line formation computations that take deviations from local thermodynamic equilibrium and hydrodynamical effects into account.

Abstract Copyright: © L. Lombardo et al. 2022

Journal keyword(s): Galaxy: abundances - Galaxy: evolution - stars: abundances - stars: Population II - stars: Population III abundances - nuclear reactions - nucleosynthesis

VizieR on-line data: <Available at CDS (J/A+A/665/A10): stars.dat table3.dat>

Simbad objects: 56

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Number of rows : 56
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 2796 Pe* 00 31 16.9147531152 -16 47 40.790991624 9.58 9.28 8.50 8.14 8.67 Fw 193 0
2 HD 4306 SB* 00 45 27.1616035344 -09 32 39.785396712 9.80 9.75 9.02 8.75   G3/5w(A) 159 0
3 CD-38 245 Pe* 00 46 36.1954514592 -37 39 33.555030480   12.733 11.929 13.39 10.996 KIIvw 224 0
4 BD-11 145 Pe* 00 48 24.3140894760 -10 41 30.892554816   11.54 10.72     KIIvw 52 0
5 HD 5426 PM* 00 55 41.0497469496 -33 45 11.452751640   10.32 9.65 9.43 8.76 G(wp) 59 0
6 HE 0057-4541 Pe* 00 59 59.2782272904 -45 24 53.424274176     14.829   13.939 ~ 9 0
7 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1359 4
8 BPS CS 22953-0003 Pe* 01 02 15.8723379360 -61 43 45.836012208   14.43 13.75 13.339 12.886 KIIvw 70 0
9 HE 0105-6141 Pe* 01 07 37.8492758736 -61 25 17.694026832   14.22 13.64 13.113 12.660 ~ 18 0
10 BPS CS 22183-0031 Pe* 01 09 05.0900915136 -04 43 21.343580436   14.24 13.62 13.178 12.724 ~ 46 0
11 BD-16 251 RG* 01 29 31.1311443552 -16 00 45.495314460 12.527 12.427 11.642 11.189 10.713 CEMP 291 0
12 HD 13979 Pe* 02 15 20.8534060680 -25 54 54.872825148   9.81 9.18     F/Gw 88 0
13 CD-22 790 Pe* 02 21 57.9369379920 -21 30 42.994815336   11.313 10.501     ~ 39 0
14 HE 0240-0807 Pe* 02 42 57.7258422024 -07 54 35.382610116   15.867 14.971 14.447 13.889 ~ 12 0
15 BPS CS 31079-0028 Pe* 03 01 00.6866893176 +06 16 31.808500140   13.900 13.211 12.713 12.190 ~ 30 0
16 CD-24 1782 Pe* 03 38 41.4850201416 -24 02 50.292102948   10.54 9.97 9.246 8.811 ~ 81 0
17 BD+06 648 Pe* 04 13 13.1126763288 +06 36 01.768985496   10.27 9.09 8.58   K0 106 0
18 BPS CS 22186-0023 RG* 04 19 45.5332495464 -36 51 35.980987284   13.57 12.84   11.925 ~ 18 0
19 HD 27928 SB* 04 22 55.1398810056 -37 15 49.243422348   10.22 9.53     Gw 52 0
20 BD-15 779 * 04 24 45.6397878168 -15 01 50.653086816   11.037 10.065     ~ 10 0
21 BD-13 899 PM* 04 30 51.4238564448 -13 34 08.141118600   10.75 10.18     ~ 3 0
22 HE 0442-1234 Pe* 04 44 51.7052109360 -12 28 45.533823744     12.914   11.672 ~ 14 0
23 HE 0516-3820 Pe* 05 18 12.9204168000 -38 17 32.704600272     14.377   13.538 ~ 7 0
24 HE 0524-2055 Pe* 05 27 04.4443239912 -20 52 42.096542448     14.013   12.937 ~ 12 0
25 TYC 5922-517-1 Pe* 05 47 20.8069100832 -17 39 40.994450640   13.42 11.92     ~ 6 0
26 TYC 4840-159-1 Pe* 07 47 15.8241428904 -04 05 46.145440464   12.18 10.55     ~ 3 0
27 TYC 8931-1111-1 Pe* 09 00 52.5868989960 -62 22 52.848219072   12.645 11.340     ~ 8 0
28 TYC 8939-2532-1 Pe* 09 08 07.5084957024 -66 07 33.896463024   12.50 11.50     ~ 4 0
29 TYC 9200-2292-1 Pe* 09 19 16.2942147144 -69 58 39.857086488   12.66 11.38     ~ 4 0
30 HD 84937 Pe* 09 48 56.0992891997 +13 44 39.326709913 8.49 8.68 8.32 7.97 7.70 F8Vm-5 795 0
31 UCAC2 1106907 Pe* 11 16 54.0105851184 -72 50 16.112976072   13.171 11.41 10.92 9.61 CEMP 10 0
32 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 40 0
33 HD 107752 Pe* 12 22 52.7183284776 +11 36 25.486007148   10.79 10.1     KIIvw 70 0
34 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 166 0
35 HD 108577 Pe* 12 28 16.8614710944 +12 20 41.089853184   10.18 9.6 9.8   KIIvw 74 0
36 BPS BS 16085-0050 Pe* 12 37 46.6781374776 +19 22 49.551755664 12.965 12.93 12.16 11.668 11.186 ~ 22 0
37 CD-23 10709A PM* 12 45 53.8523333208 -24 25 02.419072752   11.66 10.97 10.66   ~ 7 0
38 BD-13 3695 RG* 13 22 44.1122246232 -13 55 31.431021528   11.428 10.686 9.794 9.434 ~ 23 0
39 HD 122563 Pe* 14 02 31.8455084952 +09 41 09.944391876 7.47 7.10 6.19 5.37 4.79 G8:III:Fe-5 854 0
40 HD 122956 Pe* 14 05 13.0244442888 -14 51 25.455804480   8.18 7.3 6.88   G6IV/VwF6 156 0
41 TYC 9427-1414-1 Pe* 14 13 11.1788763744 -76 09 50.443206336   11.56 10.56     ~ 3 0
42 HD 126587 Pe* 14 27 00.3636631296 -22 14 38.992940592   9.88 9.60 8.75   CEMP-no 132 0
43 HD 128279 Pe* 14 36 48.5108525999 -29 06 46.612858494 8.64 8.63 8.00     Gw 194 0
44 BPS CS 30312-0100 Pe* 15 43 31.6557531288 +02 01 17.338042560   13.629 12.916 12.444 11.995 ~ 25 0
45 BD+05 3098 Pe* 15 52 17.2564983936 +05 17 44.338170732   11.26 10.56     ~ 46 0
46 BD+23 3130 Pe* 17 32 41.6247211304 +23 44 11.625460773     8.9 8.6   G0III 133 0
47 V* V2564 Oph LP? 18 04 40.0713763656 +03 46 44.716990584 9.53 8.59 7.30 6.24 5.43 F6/7V 259 0
48 BPS CS 22891-0209 Pe* 19 42 02.1802427088 -61 03 44.534898612   13.03 12.18     KIIvw 57 0
49 BPS CS 22873-0166 Pe* 20 19 22.0362485016 -61 30 15.119987544   12.818 11.802 11.52 10.57 KIIvw 55 0
50 BPS CS 22897-0008 Pe* 21 03 11.8565397504 -65 05 08.852220600   14.02 13.33     CEMP-no 70 0
51 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 34 0
52 HE 2229-4153 Pe* 22 32 49.0491790560 -41 38 25.162910736     13.322   12.447 ~ 10 0
53 CD-41 15048 Pe* 22 50 14.0199769224 -40 57 42.839116956   10.65 10.2     F8 19 0
54 HE 2252-4225 Pe* 22 54 58.5673558608 -42 09 19.386504792     14.878   13.855 ~ 23 0
55 HE 2327-5642 Pe* 23 30 37.0896973176 -56 26 14.385030648   14.590 13.881 13.425 12.948 ~ 39 0
56 BPS CS 30315-0029 Pe* 23 34 26.6960486448 -26 42 14.003379828   14.56 13.64 13.092 12.518 ~ 23 0

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