2024A&A...690A.226N


Query : 2024A&A...690A.226N

2024A&A...690A.226N - Astronomy and Astrophysics, volume 690A226 (2024/10-1)

M giants with IGRINS IV. Identification and characterisation of a NIR line of the s-element barium.

NANDAKUMAR G., RYDE N., HARTMAN H. and MACE G.

Abstract (from CDS):

Context. Neutron-capture elements represent an important nucleosynthetic channel in the study of the Galactic chemical evolution of stellar populations. For stellar populations behind significant extinction, such as those in the Galactic centre and along the Galactic plane, abundance analyses based on near-infrared (NIR) spectra are necessary. Previously, spectral lines from the neutron-capture elements, such as copper (Cu), cerium (Ce), neodymium (Nd), and ytterbium (Yb), have been identified in the H band, while yttrium (Y) lines have been identified in the K band.
Aims. Due to the scarcity of spectral lines from neutron-capture elements in the NIR, the addition of useful spectral lines from other neutron-capture elements is highly desirable. The aim of this work is to identify and characterise a spectral line suitable for abundance determination from the most commonly used s-process element, namely barium.
Methods. We observed the NIR spectra of 37 M giants in the solar neighbourhood at high spectral resolution and with a high signal-to-noise ratio using the IGRINS spectrometer on the GEMINI South telescope. The full H- and K-bands were recorded simultaneously at R = 45 000. Using a manual spectral synthesis method, we determined the fundamental stellar parameters for these stars and derived the barium abundance from the Ba line (6s5d 3D2 → 6s6p 3P2^o^) at λair = 23 253.56 Å in the K band.
Results. We demonstrate that the Ba line in the K band at 2.33 μm (λ23 253.56) is useful for abundance analyses from the spectra of M giants. The line becomes progressively weaker at higher temperatures and is only useful in M giants and the coolest K giants at supersolar metallicities.
Conclusions. We can now add Ba to the trends of the heavy elements Cu, Zn, Y, Ce, Nd, and Yb, which can be retrieved from high-resolution H- and K-band spectra. This opens up the study of nucleosynthetic channels, including the s-process and the r-process, in dust-obscured populations. Thus, these elements can be studied for heavily dust-obscured regions of the Galaxy, such as the Galactic centre.

Abstract Copyright: © The Authors 2024

Journal keyword(s): techniques: spectroscopic - stars: abundances - stars: late-type - Galaxy: abundances - solar neighborhood

Simbad objects: 38

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Number of rows : 38
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 * 30 Psc LP? 00 01 57.6194717328 -06 00 50.654004048 7.88 6.04 4.41 2.85 1.44 M3III 152 0
2 ATO J087.1710-06.0335 V* 05 48 41.0585603424 -06 02 00.877703436   14.697 12.755 12.164   M 12 0
3 HD 271773 * 05 59 44.4547750248 -72 12 11.235834180   12.45 10.94 10.45 9.24 K7 11 0
4 HD 271872 * 06 03 52.1616711672 -72 55 07.955958936   12.921 11.311 10.75 9.35 K7 17 0
5 2MASS J06052796-0553384 AB? 06 05 27.9648960218 -05 53 38.436082760   14.746 12.792 12.275   M4e 12 0
6 2MASS J06124201-0025095 LP? 06 12 42.0280938710 -00 25 09.546545022           M 10 0
7 ATO J095.6434-04.7209 LP? 06 22 34.4317657215 -04 43 15.380010643   14.701 12.731 12.089   M 13 0
8 ATO J095.8205-05.5106 LP? 06 23 16.9392638813 -05 30 38.439168667   15.100 13.120 12.312   M 12 0
9 2MASS J06520463-0047080 S*? 06 52 04.6277867395 -00 47 08.086474284   15.333 13.131 12.476   M3.0III 13 0
10 UCAC4 441-024412 * 06 55 18.0847643639 -01 48 08.045303488   13.593 11.757 11.216   M 10 0
11 2MASS J06574070-1231239 LP? 06 57 40.6978970815 -12 31 23.884289322           M 10 0
12 * mu. UMa SB* 10 22 19.7276765267 +41 29 58.337745272 6.53 4.64 3.05 1.76 0.80 M0III 331 0
13 UCAC2 11973589 Pe* 10 43 03.9598590624 -46 05 35.400191712   13.509 11.836 11.47 9.69 M 15 0
14 V* HL UMa LP* 11 07 52.7875620552 +68 21 58.853487492   9.58 8.09     M3[Swk] 58 0
15 * ome Vir LP* 11 38 27.6074536027 +08 08 03.459408149 8.46 6.93 5.36     M4.5:III 121 0
16 2MASS J12101600-4936072 LP? 12 10 16.0021496376 -49 36 07.294259808   13.652 11.836 11.45 9.74 M 14 0
17 UCAC2 9967875 * 13 40 35.1693166800 -50 40 26.159096496   13.759 11.956 11.49 9.75 M 16 0
18 2MASS J14131192-4849280 * 14 13 11.9334416454 -48 49 27.949449688           M 10 0
19 2MASS J14241044-6218367 * 14 24 10.4580909197 -62 18 36.770514108           M 9 0
20 2MASS J14260433-6219024 * 14 26 04.3377332139 -62 19 02.546266186           M 8 0
21 2MASS J14261117-6240220 * 14 26 11.1867476096 -62 40 22.109460966           M 8 0
22 2MASS J14275833-6147534 * 14 27 58.3433232835 -61 47 53.339058357           M 9 0
23 2MASS J14283733-6257279 * 14 28 37.3051752102 -62 57 27.871965246           M 8 0
24 2MASS J14291063-6317181 * 14 29 10.6535982977 -63 17 18.166871112           M 8 0
25 TYC 9010-4082-1 * 14 32 20.7204928104 -62 15 50.722234308   13.47 11.23     M 9 0
26 2MASS J14332869-6211255 * 14 33 28.6968889486 -62 11 25.535314089           M 9 0
27 2MASS J14333081-6221450 * 14 33 30.8157860091 -62 21 45.180472647           M 9 0
28 2MASS J14333688-6232028 * 14 33 36.8711220667 -62 32 02.814613879           M 9 0
29 UCAC4 138-128197 * 14 34 51.1507527961 -62 25 50.930005444   14.756 12.865 12.345   M 8 0
30 2MASS J14371958-6251344 * 14 37 19.5767999716 -62 51 34.560227025           M 9 0
31 V* RR UMi LP* 14 57 35.0095879431 +65 55 56.814643584 7.86 6.19 4.54 2.69 0.97 M4.5III 195 0
32 2MASS J15161949+0244516 RG* 15 16 19.4917445902 +02 44 51.657857508           M2.0III 12 0
33 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
34 2MASS J17584888-2351011 * 17 58 48.8974005185 -23 51 01.118947929           M 10 0
35 2MASS J18103303-1626220 * 18 10 33.0405241683 -16 26 21.958556855           M 11 0
36 UCAC4 342-124446 * 18 14 23.4671513181 -21 36 40.928048180       15.292   M 9 0
37 UCAC4 363-134678 * 18 19 15.5105926094 -17 26 22.356598776       15.216   M 14 0
38 * del02 Lyr LP* 18 54 30.2826884969 +36 53 55.031674618 7.62 5.97 4.30 2.52 0.89 M4II 251 0

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