2025A&A...703A.296M


Query : 2025A&A...703A.296M

2025A&A...703A.296M - Astronomy and Astrophysics, volume 703A296 (2025/11-1)

Understanding the origin of palladium in metal-poor stars based on the non-local thermodynamic equilibrium analysis of Pd I lines.

MASHONKINA L. and SMOGORZHEVSKII A.

Abstract (from CDS):

Context. Palladium is a poorly observed neutron-capture element. Abundance determinations for stellar samples covering a broad metallicity range are needed for a better understanding of the mechanisms of Pd synthesis during the Galaxy evolution.
Aims. We obtain accurate abundances of Pd for the Sun and a sample of metal-poor stars based on the non-local thermodynamic equilibrium (NLTE) line formation for Pd I.
Methods. We present a new comprehensive model atom of PdI. We derived the abundances of Pd, Sr, Ba, and Eu for 48 stars from the NLTE analyses of high-resolution spectra with a high signal-to-noise ratio provided by the ESO archives. The results we obtained are based on the synthetic spectrum method with one-dimensional (1D MARCS) model atmospheres.
Results. NLTE leads to weakened Pd I lines and positive NLTE abundance corrections growing from 0.2 dex for the solar lines up to 0.8 dex for the lines in the most luminous star of the sample. Depending on the treatment of inelastic collisions with hydrogen atoms, the solar NLTE abundance is log ε⊙,Pd = 1.61±0.02 to 1.70±0.02 and agrees within the error bars with the meteoritic abundance log εmet,Pd = 1.65. NLTE largely removes the discrepancies in the LTE abundances between giant and dwarf stars of similar metallicities. Palladium is tightly correlated with Eu in the -1.71 ≤ [Fe/H] ≤ -0.56 range, which indicates r- and s-process contributions to the Pd synthesis of approximately 70% and 30%, respectively. Palladium is of pure r-process origin in our two r-II stars, and a dominant contribution of the r-process to the Pd abundances is found for another two very metal-poor (VMP; [Fe/H] < -2) stars. The two VMP stars are strongly enhanced with Sr relative to Ba and Eu and also have a higher Pd. We propose that the source of the additional Sr and Pd in these stars are VMP fast-rotating massive stars.
Conclusions. NLTE is essential for obtaining the observational constraints to future models of the Galactic Pd evolution.

Abstract Copyright: © The Authors 2025

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

Simbad objects: 48

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Number of rows : 48
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 3567 PM* 00 38 31.9473242153 -08 18 33.392826667 9.54 9.70 9.23     F7/8wF3 221 0
2 HD 8724 RG* 01 26 17.5946147784 +17 07 35.123889432   9.30 8.32     G5 137 0
3 BD+20 571 Pe* 03 27 39.4522217875 +21 02 34.994793492   11.36   10.8   G0 67 0
4 CD-24 1782 Pe* 03 38 41.4850201416 -24 02 50.292102948   10.54 9.97 9.246 8.811 ~ 91 0
5 HD 22879 Pe* 03 40 22.0652879951 -03 13 01.124265616 7.146 7.222 6.667 6.346 6.016 G0VmF2 529 0
6 HD 25704 ** 04 01 44.6317980946 -57 12 24.598726799   8.65 8.10     F7V 161 0
7 HD 29907 SB* 04 38 22.3989572020 -65 24 57.594232229   10.52 9.91     F8V 106 0
8 CD-33 3337 PM* 06 54 47.8101117384 -33 44 49.024262364   9.56 9.03     F5 103 0
9 CD-57 1633 HV* 07 06 28.9516977109 -57 27 29.118927115   10.04 9.54     F7V 114 0
10 HD 59392 Pe* 07 28 03.2212916981 -38 00 41.278587469   10.17 9.7     F0V 102 0
11 CD-45 3283 PM* 07 34 18.5993129322 -45 16 42.883606401   11.08 10.43     G8V-VI 88 0
12 HD 60319 PM* 07 34 35.1077496408 +16 54 04.028098500   9.46   8.6   F8 108 0
13 * 171 Pup SB* 07 45 34.9212542040 -34 10 21.185626324   5.909 5.362     F9V 318 0
14 HD 63598 SB* 07 48 53.5375590480 -24 58 24.162494232   8.47 7.93     G2V 75 0
15 HD 76932 PM* 08 58 43.9327642391 -16 07 57.817644364 6.47 6.39 5.86     G2VFe-1.8CH-1 426 0
16 HD 83212 Pe* 09 36 19.9521173088 -20 53 14.747509716   9.582 9.177 7.83   G6/K0IIIwF7 144 0
17 HD 298986 PM* 10 17 14.8774744591 -52 29 18.694800089   10.46 10.03   9.48 F5 97 0
18 HD 97320 Pe* 11 11 00.7344001848 -65 25 37.745815656   9.769 9.269     F3V 158 0
19 HD 102200 Pe* 11 45 34.2345453384 -46 03 46.386995400   9.13 8.76     F2V 128 0
20 BD-01 2582 RG* 11 53 37.3231720128 -02 00 36.728298108   10.29 9.60     CEMP-s 125 0
21 HD 103723 PM* 11 56 36.0251513496 -21 25 09.829610868   10.554 10.091     F5/6V 87 0
22 HD 105004 PM* 12 05 24.8526164337 -26 35 43.750181317   10.96 10.39     F9 117 0
23 HD 106038 PM* 12 12 01.3688687080 +13 15 40.618559661 10.45 10.630 10.162 9.851 9.539 F6wl 204 0
24 HE 1219-0312 Pe* 12 21 34.1430245160 -03 28 39.636260184     15.940   15.043 ~ 50 0
25 HD 108317 Pe* 12 26 36.8319587208 +05 18 09.023783400       7.7   G2IVm-5 182 0
26 HD 111980 SB* 12 53 15.0529661499 -18 31 20.013189741 8.80 8.91 8.38     F7V 185 0
27 HD 113679 PM* 13 05 52.8245053407 -38 30 59.990193435   10.342 9.797     G2/3V 114 0
28 HD 120559 SB* 13 51 40.3987847839 -57 26 08.350982731 8.679 8.647 7.982 7.605 7.217 G7VFe-1.4CH-1 168 0
29 HD 121004 PM* 13 53 58.1163626566 -46 32 19.522719077   10.112 9.522     G2V 164 0
30 HD 122196 PM* 14 01 02.1249985961 -38 03 03.313496920   9.19 8.75     F0(V)w 124 0
31 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
32 HD 122956 Pe* 14 05 13.0244442888 -14 51 25.455804480   8.18 7.3 6.88   G6IV/VwF6 169 0
33 HD 126587 Pe* 14 27 00.3636631296 -22 14 38.992940592   9.88 9.60 8.75   CEMP-no 145 0
34 HD 126681 PM* 14 27 24.9094012952 -18 24 40.454425566   9.939 9.535     G3V 208 0
35 HD 128279 Pe* 14 36 48.5108525999 -29 06 46.612858494 8.64 8.63 8.00     Gw 214 0
36 HD 132475 PM* 14 59 49.7651173448 -22 00 45.815162806 8.98 9.11 8.55     F5/6V 256 1
37 HD 160617 Pe* 17 42 49.3234249010 -40 19 15.503834657   9.18 8.7 8.394 8.065 G0 220 0
38 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
39 HD 166913 PM* 18 16 25.6832938176 -59 24 11.239435980   8.66 8.23     F5/7Vw 142 0
40 HD 175179 PM* 18 54 23.2029803432 -04 36 18.621907480 9.56 9.61 9.03     G5V 135 0
41 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 166 0
42 HD 188510 PM* 19 55 09.6782304000 +10 44 27.398607828 9.30 9.41   8.5   G5V: 264 0
43 HD 189558 PM* 20 01 00.2452184673 -12 15 20.353638621   8.28 7.73     F8/G2V 202 0
44 HD 195633 PM* 20 32 23.9917043856 +06 31 03.255667608 9.05 9.03 8.52     G0Vw 155 0
45 HD 204543 * 21 29 28.2126852216 -03 30 55.353564216   9.17 8.30 7.99   F6/8(V) 144 0
46 HD 205650 PM* 21 37 26.0286639804 -27 38 06.697265704   9.59 9.00     F6V 112 0
47 HD 218857 Pe* 23 11 24.5948299440 -16 15 04.026507912   9.60 9.0     G5/8w(a) 124 0
48 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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