2026A&A...705A..38M


Query : 2026A&A...705A..38M

2026A&A...705A..38M - Astronomy and Astrophysics, volume 705A38 (2026/1-1)

Molybdenum and ruthenium in the Galactic disk: A closer look at their nucleosynthesis components.

MISHENINA T., KURTUKIAN-NIETO T., GORBANEVA T., AMARSI A.M., PSALTIS A. and PIGNATARI M.

Abstract (from CDS):

Context. The stellar origin of the elements molybdenum (Mo, Z = 42) and ruthenium (Ru, Z = 44) is still a matter of debate. Studying their abundances provides valuable insights into nucleosynthesis processes and the broader evolution of neutron-capture elements.
Aims. The aim of this work is to present new observations of Mo and Ru, together with nearby neutron-capture elements strontium (Sr) and zirconium (Zr) for a new sample of 154 giant stars, located in the Galactic disk with metallicities -1 < [Fe/H] < +0.3.
Methods. The abundances were determined under the assumption of the local thermodynamic equilibrium by fitting synthetic spectra. The abundances of Mo were derived from the Mo I lines at 5506 and 5533 Å, while the abundances of Ru were determined from Ru I lines at 4584, and 4757 Å. The abundances of Sr and Zr were measured using lines of Sr II at 4077 and 4215 Å and lines of Zr I at 5385, 6127, and 6134 Å.
Results. We derived Sr, Zr, and Mo abundances for all stars in our sample, and Ru for 110 stars. For most of the giant stars observed in this work, Mo and Ru abundances were determined for the first time. We compare our observations with the signatures from different nucleosynthesis processes.
Conclusions. Both the [Mo/Fe] and [Ru/Fe] in our stars show a decreasing trend with respect to increasing [Fe/H]. This pattern is similar to that of [Zr/Fe], whereas [Sr/Fe] exhibits a relatively flat trend with metallicity. These results are compatible with our previous measurements obtained for dwarf stars over the same metallicity range. Compared to the s-process ratios, all stars show a lower [Zr/Mo] and a higher [Ru/Mo], as expected from classical nucleosynthesis. Still, it is unclear if additional contributions from neutrino-wind components or the i-process is needed to explain the observed scatter of [Zr/Mo] and [Ru/Mo] in the Milky Way disk. Indeed, such a dispersion is consistent with the variations also seen in r-II stars at low metallicity and could therefore result from the combined contributions of r-process and s-process to galactic chemical evolution. The observed [Zr/Mo] and [Ru/Mo] scatter in r-II stars should be constrained by future investigations to define if any contributions of additional nucleosynthesis components are needed.

Abstract Copyright: © The Authors 2026

Journal keyword(s): stars: abundances - stars: late-type - Galaxy: disk - Galaxy: evolution

VizieR on-line data: <Available at CDS (J/A+A/705/A38): tablea1.dat>

Status at CDS : Tables of objects will be appraised for possible ingestion in SIMBAD.

Simbad objects: 29

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Number of rows : 29
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 * 58 Psc SB* 00 47 01.4560849248 +11 58 25.865643612   6.489 5.504     G8II 76 0
3 BD-11 160 Pe* 00 51 26.4575167968 -10 53 17.293215372   11.22 10.81     ~ 28 0
4 * 81 Cet PM* 02 37 41.8020809760 -03 23 46.225928328   6.674 5.647     K0III 97 1
5 CD-45 3283 PM* 07 34 18.5993129322 -45 16 42.883606401   11.08 10.43     G8V-VI 88 0
6 * alf Mon PM* 07 41 14.8319734511 -09 33 04.077766984 5.83 4.95 3.93 3.16 2.64 G9.5III-IIIbFe-0.5 214 0
7 HD 94028 PM* 10 51 28.1256073369 +20 16 38.965439278 8.51 8.69 8.22 7.82 7.54 F8 375 0
8 HD 120420 * 13 48 38.7352176000 +31 11 24.744142248   6.59 5.57     K0III 59 0
9 HD 120240 * 13 49 59.1348684648 -60 14 06.129621564   10.32 10.18     A3/5II/III 3 0
10 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
11 HE 1523-0901 Pe* 15 26 01.0697532504 -09 11 38.885639784   12.37 11.50 10.476 9.863 CEMP 93 0
12 * 16 Her PM* 16 15 28.6349735016 +18 48 29.117594304 7.82 6.81 5.69     K3III 67 0
13 HD 152224 PM* 16 50 43.1495843544 +32 33 13.205093472   7.182 6.158     K0III 50 0
14 HD 156874 * 17 18 48.5264966664 +28 49 22.679991408   6.658 5.680     K0III 67 0
15 BD+17 3248 HB* 17 28 14.4690179544 +17 30 35.847574776   10.02 9.34     KIIvw 239 0
16 HD 161178 * 17 37 08.8834634616 +72 27 20.858215464   6.886 5.869     G9III 79 0
17 HD 160617 Pe* 17 42 49.3234249010 -40 19 15.503834657   9.18 8.7 8.394 8.065 G0 220 0
18 HD 166578 * 18 06 40.5625937280 +64 13 17.129101692   7.63 6.68     K0 29 0
19 * 37 Dra PM* 18 15 17.0855122152 +68 45 20.942085816   7.022 5.953     K1III: 40 0
20 UCAC2 12329177 Pe* 18 30 13.5435856824 -45 55 10.139575728   12.91 12.06 11.93 11.09 CEMP 16 0
21 HD 176598 * 18 56 25.7183401176 +65 15 29.104305408   6.565 5.621     G8III 63 0
22 * 48 Dra PM* 18 56 45.0357338352 +57 48 53.339590224   6.835 5.663     K1III 66 0
23 * del Dra PM* 19 12 33.3013729052 +67 39 41.539165396 4.85 4.07 3.07 2.37 1.86 G9III 295 0
24 * eps Dra PM* 19 48 10.3504589976 +70 16 04.549073664   4.83 3.91     G7IIIbFe-1 160 0
25 TYC 8444-76-1 * 22 13 20.4894810480 -51 37 38.689403592   12.223 11.630     ~ 15 0
26 BPS CS 22892-0052 Pe* 22 17 01.6558764360 -16 39 27.051026544   14.03 13.20 13.06 12.19 KIIvw 472 0
27 HD 215030 PM* 22 41 36.0511405296 +41 32 56.847112224 7.650 6.940   5.3   G9III 63 0
28 * 14 And PM* 23 31 17.4132523248 +39 14 10.314703644   6.24   4.6   G8III 192 1
29 HD 222925 Pe* 23 45 17.6074777008 -61 54 42.835286016   9.56 9.03     ApSrEu 83 0

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