2021MNRAS.502.4210T


Query : 2021MNRAS.502.4210T

2021MNRAS.502.4210T - Mon. Not. R. Astron. Soc., 502, 4210-4226 (2021/April-2)

Effective temperatures of red supergiants estimated from line-depth ratios of iron lines in the YJ bands, 0.97-1.32µm.

TANIGUCHI D., MATSUNAGA N., JIAN M., KOBAYASHI N., FUKUE K., HAMANO S., IKEDA Y., KAWAKITA H., KONDO S., OTSUBO S., SAMESHIMA H., TAKENAKA K. and YASUI C.

Abstract (from CDS):

Determining the effective temperatures (Teff) of red supergiants (RSGs) observationally is important in many fields of stellar physics and galactic astronomy, yet some significant difficulties remain as a result of the model uncertainty, which originates mainly in the extended atmospheres of RSGs. Here we propose a line-depth ratio (LDR) method in which we use only Fe I lines. As opposed to the conventional LDR method, in which lines of multiple species are involved, this LDR method is insensitive to surface gravity effects and is expected to circumvent the uncertainty originating in the upper atmosphere of RSGs. Therefore, the LDR-Teff relationships that we calibrated empirically with red giants can be directly applied to RSGs, although various differences between the two groups of objects, for example caused by 3D non-local thermodynamic equilibrium (non-LTE) effects, need to be kept in mind. Using the near-infrared YJ-band spectra of nine well-known solar-metallicity red giants observed with the WINERED high-resolution spectrograph, we selected 12 pairs of Fe I lines that were the least contaminated with other lines. After applying their LDR-Teff relation to 10 nearby RSGs, the resulting Teff with an internal precision of 30-70 K shows good agreement with previous observational results assuming 1D LTE and with the Geneva stellar evolution model. We found no evidence of significant systematic bias caused by various differences, including those in the size of the non-LTE effects, between red giants and RSGs, except for one line pair that we rejected because the non-LTE effects may be as large as ∼250 K. Nevertheless, it is difficult to evaluate the systematic bias, and further study is required, for example including the 3D non-LTE calculations of all the lines involved.

Abstract Copyright: © The Author(s) 2021. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): techniques: spectroscopic - stars: atmospheres - stars: fundamental parameters - stars: late-type - supergiants - infrared: stars

Errata: erratum vol. 512, p. 2669 (2022)

Simbad objects: 37

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Number of rows : 37
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 * c And PM* 02 19 16.7969275675 +47 22 47.913234056   5.310 5.310     A0V 71 0
2 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
3 * alf Cet LP? 03 02 16.77307 +04 05 23.0596 6.10 4.17 2.53 1.18 0.02 M1.5IIIa 480 1
4 HD 19065 * 03 07 18.9785125632 +64 03 27.478027080   5.859 5.877     B9V 56 0
5 HD 21402 PM* 03 28 20.7005730600 +33 48 27.207327888 5.840 5.770 5.730     A2V 44 0
6 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
7 HD 29573 ** 04 38 53.5501496352 -12 07 23.068127568   5.065 5.002     A0V 99 0
8 V* NO Aur s*r 05 40 42.0497751264 +31 55 14.197536156 10.52 8.30 6.21 4.43 3.02 M2Iab 152 1
9 * omi Aur * 05 45 54.0419582136 +49 49 34.575758364   5.495 5.460     A2VpCr 130 0
10 * 136 Tau SB* 05 53 19.6462510620 +27 36 44.142990481   4.539 4.552     A0V+A0V 92 0
11 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1789 0
12 * bet Aur SB* 05 59 31.7229284 +44 56 50.757259 1.97 1.93 1.90 1.82 1.83 A1IV-Vp 433 1
13 V* TV Gem s*r 06 11 51.4142883048 +21 52 05.653085916 10.58 8.81 6.56 4.65 3.17 M0-M1.5Iab 181 0
14 * 6 Gem s*r 06 12 19.0988355816 +22 54 30.653107164 11.11 8.63 6.39 4.55 3.07 M1-M2Ia-Iab 187 0
15 * psi01 Aur s*r 06 24 53.9015502096 +49 17 16.411221960 8.85 6.67 4.75 3.36 2.29 K5-M1Iab-Ib 178 0
16 * 41 Gem s*r 07 00 15.8233724160 +16 04 44.385187008 9.09 7.32 5.69 4.44 3.59 K3-Ib 110 0
17 * 21 Lyn PM* 07 26 42.8522129445 +49 12 41.497452754   4.594 4.610     A0.5Vs 121 0
18 * kap Gem ** 07 44 26.8438122013 +24 23 52.787290890 5.19 4.49 3.57 2.86 2.41 G8III-IIIb 308 0
19 * bet Gem PM* 07 45 18.94987 +28 01 34.3160 3.00 2.14 1.14 0.39 -0.11 K0IIIb 1150 2
20 * 50 Cnc PM* 08 46 56.0189914848 +12 06 35.830080180   5.992 5.885 7.20 5.76 A1Vp 99 0
21 * alf Hya * 09 27 35.24270 -08 39 30.9583 5.14 3.42 1.97 0.93 0.16 K3IIIa 455 1
22 * eps Leo V* 09 45 51.0736168507 +23 46 27.313597604 4.23 3.79 2.98 2.36 1.93 G1IIIa 354 0
23 * mu. Leo PM* 09 52 45.8170136628 +26 00 25.024269924 6.50 5.10 3.88 2.97 2.39 K2IIIbCN1Ca1 479 0
24 * 39 UMa PM* 10 43 43.3264670520 +57 11 57.118841016   5.744 5.782     A0III 68 0
25 * bet UMa PM* 11 01 50.4797515135 +56 22 56.761138187 2.35 2.35 2.37 2.31 2.35 A1IVps 462 0
26 * gam UMa Em* 11 53 49.8473166 +53 41 41.135025 2.440 2.450 2.440 2.44 2.47 A0V 417 0
27 * b Vir * 11 59 56.9134992240 +03 39 18.736620984   5.346 5.345   5.34 A0V 73 0
28 * eps Vir PM* 13 02 10.5970152536 +10 57 32.935398266 4.45 3.71 2.79 2.16 1.71 G8III-IIIb 574 0
29 * 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
30 * alf CrB SB* 15 34 41.2684881676 +26 42 52.866000089 2.19 2.22 2.24 2.21 2.25 A1IV 499 0
31 * del Oph PM* 16 14 20.7390218758 -03 41 39.572826363 6.30 4.34 2.75 1.46 0.43 M0.5III 377 0
32 HD 156653 * 17 18 04.9427402976 +17 19 04.382069304   6.002 5.992     A1V 46 0
33 * ksi Cyg SB* 21 04 55.8599363125 +43 55 40.272058234 7.17 5.39 3.73 2.55 1.63 K4.5Ib-II 324 0
34 * zet Cep s*r 22 10 51.2777055617 +58 12 04.542602641 6.62 4.90 3.35 2.27 1.49 K1.5Ib 295 0
35 V* V424 Lac s*r 22 56 25.9983901008 +49 44 00.758688324 8.66 6.71 4.94 3.59 2.54 K5Ib 166 0
36 V* V809 Cas s*r 23 19 23.7722967840 +62 44 23.192795652   8.932 6.671     K4.5Ib 76 0
37 HD 222109 ** 23 37 32.04280 +44 25 44.3723           B8V 76 0

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