2023A&A...675A..23N


Query : 2023A&A...675A..23N

2023A&A...675A..23N - Astronomy and Astrophysics, volume 675A23 (2023/7-1)

M giants with IGRINS I. Stellar parameters and α-abundance trends of the solar neighborhood population.

NANDAKUMAR G., RYDE N., CASAGRANDE L. and MACE G.

Abstract (from CDS):

Context. Cool stars, such as M giants, can only be analyzed in the near-infrared (NIR) regime due to the ubiquitous titanium oxide features in optical spectra of stars with Teff < 4000 K. In dust-obscured regions, the inner bulge and Galactic center region, the intrinsically bright M giants observed in the NIR are an optimal option for studying stellar abundances and the chemical evolution of stellar populations. Because of the uncertainties in photometric methods, a method for determining the stellar parameters for M giants from the NIR spectra themselves is needed.
Aims. We develop a method for determining the stellar parameters for M giants from the NIR spectra. We validate the method by deriving the stellar parameters for nearby well-studied M giants with spectra from the spectral library of the Immersion GRating INfrared Spectrograph (IGRINS). We demonstrate the accuracy and precision of our method by determining the stellar parameters and α-element trends versus metallicity for solar neighborhood M giants.
Methods. We carried out new observations of 44 M giant stars with IGRINS mounted on the Gemini South telescope. We also obtained the full H and K band IGRINS spectra of six nearby well-studied M giants at a spectral resolving power of R = 45 000 from the IGRINS spectral library. We used the tool called spectroscopy made easy in combination with one-dimensional (1D) model atmospheres in a radiative and convective scheme (MARCS) stellar atmosphere models to model the synthetic spectrum that fits the observed spectrum best.
Results. The effective temperatures that we derive from our new method (tested for 3400 ≲ Teff ≲ 4000 K here) agree excellently with those of the six nearby well-studied M giants, which indicates that the accuracy is indeed high. For the 43 solar neighborhood M giants, our Teff, log g, [Fe/H], ξmicro, [C/Fe], [N/Fe], and [O/Fe] agree with APOGEE with mean differences and a scatter (our method - APOGEE) of -67±33 K, -0.31±0.15 dex, 0.02±0.05 dex, 0.22±0.13 km s–1, -0.05±0.06 dex, 0.06±0.06 dex, and 0.02±0.09 dex, respectively. Furthermore, the tight offset with a small dispersion compared to the APOGEE Teff indicates a high precision in our derived temperatures and those derived from the APOGEE pipeline. The typical uncertainties in the stellar parameters are found to be ±100 K in Teff, ±0.2 dex in log g, ±0.1 dex in [Fe/H], and ±0.1 km s–1 in ξmicro. The α-element trends versus metallicity for Mg, Si, Ca, and Ti are consistent with the APOGEE DR17 trends for the same stars and with the GILD optical trends. We also find a clear enhancement in the abundances for thick-disk stars.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: fundamental parameters - stars: abundances - stars: late-type - techniques: spectroscopic - Galaxy: abundances

VizieR on-line data: <Available at CDS (J/A+A/675/A23): table3.dat tablea6.dat tablea7.dat tablea8.dat tablea9.dat>

Simbad objects: 52

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Number of rows : 52
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 2MASS J06035110-7456029 LP? 06 03 51.1172477208 -74 56 03.001938288   13.693 11.907 11.59 9.51 M 13 0
5 HD 271872 * 06 03 52.1616711672 -72 55 07.955958936   12.921 11.311 10.75 9.35 K7 17 0
6 2MASS J06052796-0553384 AB? 06 05 27.9648960218 -05 53 38.436082760   14.746 12.792 12.275   M4e 12 0
7 UCAC4 423-012604 * 06 07 40.9641612557 -05 30 33.220107636       15.730   M 7 0
8 2MASS J06124201-0025095 LP? 06 12 42.0280938710 -00 25 09.546545022           M 10 0
9 2MASS J06140107-0641072 AB? 06 14 01.0737260375 -06 41 07.197339996   15.379 13.202 12.493   M3.0III 10 0
10 2MASS J06143705-0551064 AB? 06 14 37.0537323146 -05 51 06.341367528   14.763 12.626 12.061   M3e 10 0
11 MSX LMC 1619 LP? 06 17 11.6137597464 -72 59 32.028860688   12.665 11.014     M 13 0
12 ATO J095.6434-04.7209 LP? 06 22 34.4317657215 -04 43 15.380010643   14.701 12.731 12.089   M 13 0
13 ATO J095.8205-05.5106 LP? 06 23 16.9392638813 -05 30 38.439168667   15.100 13.120 12.312   M 12 0
14 2MASS J06520463-0047080 S*? 06 52 04.6277867395 -00 47 08.086474284   15.333 13.131 12.476   M3.0III 13 0
15 UCAC4 441-024412 * 06 55 18.0847643639 -01 48 08.045303488   13.593 11.757 11.216   M 10 0
16 2MASS J06574070-1231239 LP? 06 57 40.6978970815 -12 31 23.884289322           M 10 0
17 * mu. UMa SB* 10 22 19.7276765267 +41 29 58.337745272 6.53 4.64 3.05 1.76 0.80 M0III 331 0
18 UCAC2 11973589 Pe* 10 43 03.9598590624 -46 05 35.400191712   13.509 11.836 11.47 9.69 M 15 0
19 UCAC2 1026570 * 11 04 25.4177251248 -73 18 06.994008324   13.834 11.927 11.51 9.86 M 11 0
20 V* HL UMa LP* 11 07 52.7875620552 +68 21 58.853487492   9.58 8.09     M3[Swk] 58 0
21 * ome Vir LP* 11 38 27.6074536027 +08 08 03.459408149 8.46 6.93 5.36     M4.5:III 121 0
22 2MASS J12101600-4936072 LP? 12 10 16.0021496376 -49 36 07.294259808   13.652 11.836 11.45 9.74 M 14 0
23 UCAC2 9967875 * 13 40 35.1693166800 -50 40 26.159096496   13.759 11.956 11.49 9.75 M 16 0
24 2MASS J14131192-4849280 * 14 13 11.9334416454 -48 49 27.949449688           M 10 0
25 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
26 2MASS J14240039-6252516 * 14 24 00.3690154746 -62 52 51.714672393           M 7 0
27 2MASS J14241044-6218367 * 14 24 10.4580909197 -62 18 36.770514108           M 9 0
28 2MASS J14260433-6219024 * 14 26 04.3377332139 -62 19 02.546266186           M 8 0
29 2MASS J14261117-6240220 * 14 26 11.1867476096 -62 40 22.109460966           M 8 0
30 2MASS J14275833-6147534 * 14 27 58.3433232835 -61 47 53.339058357           M 9 0
31 2MASS J14283733-6257279 * 14 28 37.3051752102 -62 57 27.871965246           M 8 0
32 2MASS J14291063-6317181 * 14 29 10.6535982977 -63 17 18.166871112           M 8 0
33 2MASS J14311520-6145468 * 14 31 15.20184 -61 45 46.8144           M 7 0
34 TYC 9010-4082-1 * 14 32 20.7204928104 -62 15 50.722234308   13.47 11.23     M 9 0
35 2MASS J14332169-6302108 * 14 33 21.6684676665 -63 02 10.882933692           M 8 0
36 2MASS J14332869-6211255 * 14 33 28.6968889486 -62 11 25.535314089           M 9 0
37 2MASS J14333081-6221450 * 14 33 30.8157860091 -62 21 45.180472647           M 9 0
38 2MASS J14333688-6232028 * 14 33 36.8711220667 -62 32 02.814613879           M 9 0
39 UCAC4 138-128197 * 14 34 51.1507527961 -62 25 50.930005444   14.756 12.865 12.345   M 8 0
40 2MASS J14360142-6228561 LP? 14 36 01.4408662004 -62 28 56.228663242           M 8 0
41 2MASS J14360935-6309399 * 14 36 09.3692894053 -63 09 39.990432015           M 7 0
42 2MASS J14371958-6251344 * 14 37 19.5767999716 -62 51 34.560227025           M 9 0
43 2MASS J14375085-6237526 * 14 37 50.8535076094 -62 37 52.758993772           M 8 0
44 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
45 2MASS J15161949+0244516 RG* 15 16 19.4917445902 +02 44 51.657857508           M2.0III 12 0
46 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
47 2MASS J17584888-2351011 * 17 58 48.8974005185 -23 51 01.118947929           M 10 0
48 2MASS J18103303-1626220 * 18 10 33.0405241683 -16 26 21.958556855           M 11 0
49 UCAC4 342-124446 * 18 14 23.4671513181 -21 36 40.928048180       15.292   M 9 0
50 UCAC4 363-134678 * 18 19 15.5105926094 -17 26 22.356598776       15.216   M 14 0
51 2MASS J18522108-3022143 Pe* 18 52 21.0940999992 -30 22 14.349547020           M 12 0
52 * 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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