2024A&A...691A.220F


Query : 2024A&A...691A.220F

2024A&A...691A.220F - Astronomy and Astrophysics, volume 691A220 (2024/11-1)

Chemical Evolution of R-process Elements in Stars (CERES) II. The impact of stellar evolution and rotation on light and heavy elements.

FERNANDES DE MELO R., LOMBARDO L., ALENCASTRO PULS A., ROMANO D., HANSEN C.J., TSIATSIOU S. and MEYNET G.

Abstract (from CDS):

Context. Carbon, nitrogen, and oxygen are the most abundant elements throughout the universe, after hydrogen and helium. Studying these elements in low-metallicity stars can provide crucial information on the chemical composition in the early Galaxy and possible internal mixing processes that can alter the surface composition of the stars.
Aims. This work aims to investigate the chemical abundance patterns for CNO elements and Li in a homogeneously analyzed sample of 52 metal-poor halo giant stars. From these results, we have been able to determine whether internal mixing processes have taken place in these stars.
Methods. We used high-resolution spectra with a high signal-to-noise ratio (S/N) to carry out a spectral synthesis to derive detailed C, N, O, and Li abundances for a sample of stars with metallicities in the range of -3.58 ≤ [Fe/H] ≤ -1.79 dex. Our study was based on the assumption of one-dimensional (1D) local thermodynamic equilibrium (LTE) atmospheres.
Results. Based on carbon and nitrogen abundances, we investigated the deep mixing taking place within stars along the red giant branch (RGB). The individual abundances of carbon decrease towards the upper RGB while nitrogen shows an increasing trend, indicating that carbon has been converted into nitrogen. No signatures of ON-cycle processed material were found for the stars in our sample. We computed a set of galactic chemical evolution (GCE) models, implementing different sets of massive star yields, both with and without including the effects of stellar rotation on nucleosynthesis. We confirm that stellar rotation is necessary to explain the highest [N/Fe] and [N/O] ratios observed in unmixed halo stars. The predicted level of N enhancement varies sensibly in dependence of the specific set of yields that are adopted. For stars with stellar parameters similar to those of our sample, heavy elements such as Sr, Y, and Zr appear to have unchanged abundances despite the stellar evolution mixing processes.
Conclusions. The unmixed RGB stars provide very useful constraints on chemical evolution models of the Galaxy. As they are more luminous than unevolved (main sequence and turnoff) stars, they also allow for stars to be probed at greater distances. The stellar CN-cycle clearly changes the atmospheric abundances of the lighter elements, but no changes were detected with respect to the heavy elements.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: abundances - stars: atmospheres - stars: evolution - stars: Population II - galaxy: halo

Simbad objects: 54

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Number of rows : 54
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 2796 Pe* 00 31 16.9147531152 -16 47 40.790991624 9.58 9.28 8.50 8.14 8.67 Fw 203 0
2 HD 4306 SB* 00 45 27.1616035344 -09 32 39.785396712 9.80 9.75 9.02 8.75   G3/5w(A) 168 0
3 BD-11 145 Pe* 00 48 24.3140894760 -10 41 30.892554816   11.54 10.72     KIIvw 60 0
4 HD 5426 PM* 00 55 41.0497469496 -33 45 11.452751640   10.32 9.65 9.43 8.76 G(wp) 67 0
5 HE 0057-4541 Pe* 00 59 59.2782272904 -45 24 53.424274176     14.829   13.939 ~ 13 0
6 BPS CS 22953-0003 Pe* 01 02 15.8723379360 -61 43 45.836012208   14.43 13.75 13.339 12.886 KIIvw 78 0
7 HE 0105-6141 Pe* 01 07 37.8492758736 -61 25 17.694026832   14.22 13.64 13.113 12.660 ~ 22 0
8 BPS CS 22183-0031 Pe* 01 09 05.0900915136 -04 43 21.343580436   14.24 13.62 13.178 12.724 ~ 52 0
9 HD 13979 Pe* 02 15 20.8534060680 -25 54 54.872825148   9.81 9.18     F/Gw 97 0
10 CD-22 790 Pe* 02 21 57.9369379920 -21 30 42.994815336   11.313 10.501     ~ 42 0
11 HE 0240-0807 Pe* 02 42 57.7258422024 -07 54 35.382610116   15.867 14.971 14.447 13.889 ~ 18 0
12 BPS CS 31079-0028 Pe* 03 01 00.6866893176 +06 16 31.808500140   13.900 13.211 12.713 12.190 ~ 39 0
13 CD-24 1782 Pe* 03 38 41.4850201416 -24 02 50.292102948   10.54 9.97 9.246 8.811 ~ 91 0
14 BD+06 648 Pe* 04 13 13.1126763288 +06 36 01.768985496   10.27 9.09 8.58   K0 117 0
15 BPS CS 22186-0023 RG* 04 19 45.5332495464 -36 51 35.980987284   13.57 12.84   11.925 ~ 23 0
16 HD 27928 SB* 04 22 55.1398810056 -37 15 49.243422348   10.22 9.53     Gw 61 0
17 BD-15 779 * 04 24 45.6397878168 -15 01 50.653086816   11.037 10.065     ~ 14 0
18 BD-13 899 PM* 04 30 51.4238564448 -13 34 08.141118600   10.75 10.18     ~ 6 0
19 HE 0442-1234 Pe* 04 44 51.7052109360 -12 28 45.533823744     12.914   11.672 ~ 17 0
20 HE 0516-3820 Pe* 05 18 12.9204168000 -38 17 32.704600272     14.377   13.538 ~ 12 0
21 HE 0524-2055 Pe* 05 27 04.4443239912 -20 52 42.096542448     14.013   12.937 ~ 18 0
22 TYC 5922-517-1 Pe* 05 47 20.8069100832 -17 39 40.994450640   13.42 11.92     ~ 9 0
23 TYC 4840-159-1 Pe* 07 47 15.8241428904 -04 05 46.145440464   12.18 10.55     ~ 6 0
24 TYC 8931-1111-1 Pe* 09 00 52.5868989960 -62 22 52.848219072   12.645 11.340     ~ 13 0
25 TYC 8939-2532-1 Pe* 09 08 07.5084957024 -66 07 33.896463024   12.50 11.50     ~ 9 0
26 TYC 9200-2292-1 Pe* 09 19 16.2942147144 -69 58 39.857086488   12.66 11.38     ~ 9 0
27 UCAC2 1106907 Pe* 11 16 54.0105851184 -72 50 16.112976072   13.171 11.41 10.92 9.61 CEMP 14 0
28 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 50 0
29 HD 107752 Pe* 12 22 52.7183284776 +11 36 25.486007148   10.79 10.1     KIIvw 83 0
30 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 182 0
31 HD 108577 Pe* 12 28 16.8614710944 +12 20 41.089853184   10.18 9.6 9.8   KIIvw 84 0
32 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
33 CD-23 10709A PM* 12 45 53.8523333208 -24 25 02.419072752   11.66 10.97 10.66   ~ 10 0
34 BD-13 3695 RG* 13 22 44.1122246232 -13 55 31.431021528   11.428 10.686 9.794 9.434 ~ 35 0
35 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
36 HD 122956 Pe* 14 05 13.0244442888 -14 51 25.455804480   8.18 7.3 6.88   G6IV/VwF6 169 0
37 TYC 9427-1414-1 Pe* 14 13 11.1788763744 -76 09 50.443206336   11.56 10.56     ~ 7 0
38 HD 126587 Pe* 14 27 00.3636631296 -22 14 38.992940592   9.88 9.60 8.75   CEMP-no 145 0
39 HD 128279 Pe* 14 36 48.5108525999 -29 06 46.612858494 8.64 8.63 8.00     Gw 214 0
40 BPS CS 30312-0100 Pe* 15 43 31.6557531288 +02 01 17.338042560   13.629 12.916 12.444 11.995 ~ 31 0
41 BD+05 3098 Pe* 15 52 17.2564983936 +05 17 44.338170732   11.26 10.56     ~ 49 0
42 BD+23 3130 Pe* 17 32 41.6247211304 +23 44 11.625460773     8.9 8.6   G0III 144 0
43 V* V2564 Oph LP? 18 04 40.0713763656 +03 46 44.716990584 9.53 8.59 7.30 6.24 5.43 F6/7V 274 0
44 BPS CS 22891-0209 Pe* 19 42 02.1802427088 -61 03 44.534898612   13.03 12.18     KIIvw 64 0
45 BD-18 5550 Pe* 19 58 49.7371417608 -18 12 11.140126164 10.18 10.03 9.35 9.04 8.74 CEMP-no 185 0
46 BPS CS 22873-0166 Pe* 20 19 22.0362485016 -61 30 15.119987544   12.818 11.802 11.52 10.57 KIIvw 62 0
47 BPS CS 22897-0008 Pe* 21 03 11.8565397504 -65 05 08.852220600   14.02 13.33     CEMP-no 80 0
48 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 43 0
49 HE 2229-4153 Pe* 22 32 49.0491790560 -41 38 25.162910736     13.322   12.447 ~ 17 0
50 CD-41 15048 Pe* 22 50 14.0199769224 -40 57 42.839116956   10.65 10.2     F8 25 0
51 HE 2252-4225 Pe* 22 54 58.5673558608 -42 09 19.386504792     14.878   13.855 ~ 30 0
52 HE 2327-5642 Pe* 23 30 37.0896973176 -56 26 14.385030648   14.590 13.881 13.425 12.948 ~ 51 0
53 BPS CS 30315-0029 Pe* 23 34 26.6960486448 -26 42 14.003379828   14.56 13.64 13.092 12.518 ~ 32 0
54 NAME Local Group GrG ~ ~           ~ 9325 0

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