2022A&A...663A..70F


Query : 2022A&A...663A..70F

2022A&A...663A..70F - Astronomy and Astrophysics, volume 663A70-70 (2022/7-1)

Correlations of r-process elements in very metal-poor stars as clues to their nucleosynthesis sites.

FAROUQI K., THIELEMANN F.-K., ROSSWOG S. and KRATZ K.-L.

Abstract (from CDS):


Aims. Various nucleosynthesis studies have pointed out that the r-process elements in very metal-poor (VMP) halo stars might have different origins. By means of familiar concepts from statistics (correlations, cluster analysis, and rank tests of elemental abundances), we look for causally correlated elemental abundance patterns and attempt to link them to astrophysical events. Some of these events produce the r-process elements jointly with iron, while others do not have any significant iron contribution. We try to (a) characterize these different types of events by their abundance patterns and (b) identify them among the existing set of suggested r-process sites.
Methods. The Pearson and Spearman correlation coefficients were used in order to investigate correlations among r-process elements (X,Y) as well as their relation to iron (Fe) in VMP halo stars. We gradually tracked the evolution of those coefficients in terms of the element enrichments [X/Fe] or [X/Y] and the metallicity [Fe/H]. This approach, aided by cluster analysis to find different structures of abundance patterns and rank tests to identify whether several events contributed to the observed pattern, is new and provides deeper insights into the abundances of VMP stars.
Results. In the early stage of our Galaxy, at least three r-process nucleosynthesis sites have been active. The first two produce and eject iron and the majority of the lighter r-process elements. We assign them to two different types of core-collapse events, not identical to regular core-collapse supernovae (CCSNe), which produce only light trans-Fe elements. The third category is characterized by a strong r-process and is responsible for the major fraction of the heavy main r-process elements without a significant coproduction of Fe. It does not appear to be connected to CCSNe, in fact most of the Fe found in the related r-process enriched stars must come from previously occurring CCSNe. The existence of actinide boost stars indicates a further division among strong r-process sites. We assign these two strong r-process sites to neutron star mergers without fast black hole formation and to events where the ejecta are dominated by black hole accretion disk outflows. Indications from the lowest-metallicity stars hint at a connection with massive single stars (collapsars) forming black holes in the early Galaxy.

Abstract Copyright: © K. Farouqi et al. 2022

Journal keyword(s): nuclear reactions - nucleosynthesis - abundances - stars: abundances - supernovae: general - Galaxy: halo - methods: statistical

Simbad objects: 47

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Number of rows : 47
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 HE 0010-3422a HB* 00 12 55.9165648224 -34 05 44.432616768   15.6 15.5     ~ 7 1
2 BPS CS 22882-0001 HB* 00 20 25.2919782216 -31 39 04.069467288   15.22 14.82     ~ 23 0
3 BPS CS 29497-0004 Pe* 00 28 06.9155612016 -26 03 04.269055032   14.76 14.07 13.583 13.116 ~ 64 0
4 SKB 2 Pe* 00 41 39.8197621944 -26 18 54.460585116   13.332 12.184 12.072 11.321 CEMP-s 92 0
5 SB 960 Pe* 00 44 03.5698629048 -13 55 26.268999384   12.69 12.15 11.806 11.483 CEMP-s 114 0
6 HE 0058-0244 Pe* 01 00 53.0234702616 -02 28 19.950391884   14.42 13.73 13.331 12.942 CEMP-r/s 40 0
7 BPS CS 22953-0003 Pe* 01 02 15.8723379360 -61 43 45.836012208   14.43 13.75 13.339 12.886 KIIvw 78 0
8 HD 6268 Pe* 01 03 18.1716378504 -27 52 49.953768852   9.725 9.046 8.601   F/Gw 166 0
9 HE 0105-6141 Pe* 01 07 37.8492758736 -61 25 17.694026832   14.22 13.64 13.113 12.660 ~ 22 0
10 BD-16 251 RG* 01 29 31.1311443552 -16 00 45.495314460 12.527 12.427 11.642 11.189 10.713 CEMP 318 0
11 HD 11544 * 01 54 56.3724512256 +56 34 56.918915868   7.955 6.827     G2Ib 59 0
12 HE 0240-0807 Pe* 02 42 57.7258422024 -07 54 35.382610116   15.867 14.971 14.447 13.889 ~ 18 0
13 HE 0243-3044 Pe* 02 45 16.4464212312 -30 32 02.118309504   17.11 16.10     CEMP-rs 15 0
14 BPS CS 31079-0028 Pe* 03 01 00.6866893176 +06 16 31.808500140   13.900 13.211 12.713 12.190 ~ 39 0
15 HE 0315+0000 Pe* 03 17 39.0100103112 +00 11 04.600281192     15.516   14.506 F5 15 0
16 TYC 5329-1927-1 Pe* 05 06 20.1241488048 -13 44 21.982874532   13.06 11.71     CEMP 13 0
17 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
18 BD-07 2674 Pe* 08 58 05.8480558056 -08 09 17.382965652   11.18 10.26     CEMP 11 0
19 TYC 3814-1598-1 Pe* 09 54 42.7718004504 +52 46 41.559838968   11.19 10.10     ~ 32 0
20 HE 1127-1143 Pe* 11 29 50.6275439136 -12 00 12.581828208     15.885 15.434 15.002 ~ 17 0
21 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 50 0
22 HD 107752 Pe* 12 22 52.7183284776 +11 36 25.486007148   10.79 10.1     KIIvw 83 0
23 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 182 0
24 HD 110184 SB* 12 40 14.0781612216 +08 31 38.057301300 10.20 9.45 8.27 8.52   KIIvw 153 0
25 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
26 HD 115444 Pe* 13 16 42.4590842616 +36 22 52.692135420   9.77 8.97 8.3 7.88 G9V 252 0
27 2MASS J13262814+2138429 Pe* 13 26 28.1414236104 +21 38 42.851996448   13.26 12.6 12.113 11.657 ~ 12 0
28 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
29 TYC 7814-133-1 Pe* 14 32 53.3360210280 -41 25 49.477241028   11.76 11.08     ~ 15 0
30 HE 1523-0901 Pe* 15 26 01.0697532504 -09 11 38.885639784   12.37 11.50 10.476 9.863 CEMP 93 0
31 LP 625-44 Pe* 16 43 14.0377103880 -01 55 30.411443424   12.84 11.68     CEMP-s 111 0
32 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 166 0
33 UCAC4 392-119337 Pe* 20 03 22.5355575550 -11 42 02.781717289   12.662 11.877 11.703   ~ 17 0
34 UCAC2 31779418 Pe* 20 38 43.1848979784 -00 23 32.761814352   13.726 12.731 12.51 11.57 CEMP 34 0
35 BD-15 5781 Pe* 20 45 34.5446785080 -14 31 15.154963788   11.57 10.83     KIIvw 56 0
36 HE 2138-3336 Pe* 21 41 20.3876075232 -33 22 29.628166296   15.42 14.80 14.65   CEMP-s 7 0
37 HE 2206-2245 Pe* 22 09 09.4304757432 -22 30 16.235826840     15.534   14.616 ~ 7 0
38 HE 2208-1239 Pe* 22 10 53.4450437784 -12 24 27.003628548   12.54 11.72 11.66   CEMP-rs 12 0
39 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
40 HE 2224+0143 Pe* 22 27 23.1215289240 +01 58 33.066485508   14.54 13.83 13.208 12.733 ~ 23 0
41 BPS CS 29491-0069 Pe* 22 31 02.1859040712 -32 38 36.526573572   13.72 13.1 12.654 12.175 ~ 43 0
42 HE 2252-4225 Pe* 22 54 58.5673558608 -42 09 19.386504792     14.878   13.855 ~ 30 0
43 HE 2258-6358 Pe* 23 01 48.6559441632 -63 42 25.117355556   15.42 14.30 14.07   CEMP-s 14 0
44 HE 2327-5642 Pe* 23 30 37.0896973176 -56 26 14.385030648   14.590 13.881 13.425 12.948 ~ 51 0
45 BPS CS 30315-0029 Pe* 23 34 26.6960486448 -26 42 14.003379828   14.56 13.64 13.092 12.518 ~ 32 0
46 BPS CS 29499-0003 Pe* 23 39 42.9584819976 -26 58 55.613762436     14.29     ~ 13 0
47 GRB 190425 GWE ~ ~           ~ 438 0

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