2025ApJ...991..173D


Query : 2025ApJ...991..173D

2025ApJ...991..173D - Astrophys. J., 991, 173 (2025/October-1)

A Spectroscopic Hunt for Post-Red Supergiants in the Large Magellanic Cloud. II. Turbulent Line Broadening in the Spectra of LMC Yellow Supergiants.

DORN-WALLENSTEIN T.Z., CHEN K.M., WU S.C., GOLDBERG J.A., O'GRADY A.J.G., MANN A.T. and DON-WALLANCHEZ P.I.

Abstract (from CDS):

Massive stars in the Hertzsprung gap are a mixed population of objects in short-lived evolutionary phases: yellow supergiants (YSGs) evolving toward the red supergiant (RSG) phase, partially stripped post-RSGs, and other, rarer outcomes of stellar evolution. Studies of sufficiently large samples of these objects can constrain massive star structure and evolution during these poorly understood phases. As part of our ongoing program searching for post-RSGs, we characterized the spectral line profiles of 32 YSGs in the Large Magellanic Cloud using high-resolution spectra obtained with the Magellan Inamori Kyocera Echelle spectrograph on the Magellan 2/Clay telescope at Las Campanas Observatory. We find that the line profiles are strongly broadened by turbulent photospheric motion. After fitting the profiles to measure microturbulent and macroturbulent velocities, we identify two groups within our sample that are separated by the ratio of the two velocity scales. In both groups, the macroturbulent velocity ζRT scales with stellar properties such as effective temperature. Additionally, we find statistically significant correlations between the macroturbulent velocity and other possible probes of large-scale photospheric motions: line profile asymmetry, as well as the amplitude and quality factor of the stochastic low frequency variability measured from Transiting Exoplanet Survey Satellite lightcurves. These correlations differ between the two groups of YSGs. Finally, we construct 1D evolutionary models of YSGs in both pre- and post-RSG phases, and find reasonable agreement between the convective velocities in these models and our measured microturbulent velocities. However, the macroturbulent velocities are much higher than the convective velocities in the models.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Late-type supergiant stars - Stellar mass loss - High resolution spectroscopy - Observational astronomy - Large Magellanic Cloud - Massive stars - Yellow hypergiant stars - Evolved stars - Hertzsprung gap - Stellar evolution - Stellar structures

Simbad objects: 47

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Number of rows : 47
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 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
2 HD 268687 s*y 04 50 55.8562324872 -69 25 52.504903884 11.33 11.12 10.730 10.70 10.145 F6Ia 38 0
3 SP77 31-16 LP* 04 54 36.8435054448 -69 20 22.179167376   12.25 10.89 10.39   K/M 26 0
4 HD 268819 s*y 04 55 32.4586567536 -69 57 45.085303296 10.97 10.58 10.08 9.72 9.541 F5Ia 60 0
5 HD 268727 sg* 04 56 39.9075220656 -66 44 36.703812732   11.67 11.59     A0Ia 24 0
6 HD 268828 * 04 56 40.0088781408 -69 41 56.356809000   12.45 11.80 11.39   K5 18 0
7 RM 1-77 * 04 56 49.4338837056 -69 48 31.512451212   13.10 11.55 10.80   M: 17 0
8 HD 268865 * 04 59 43.5492169800 -68 31 22.779485148   12.17 11.46 11.05   K0 19 0
9 SV* HV 883 cC* 05 00 07.5644790720 -68 27 00.064228464 14.033 13.86 11.63 11.35 10.91 F8/G0Ia 90 0
10 HD 268971 sg* 05 01 45.1929226848 -70 35 52.163553012   11.66 11.615   11.490 A0Ia 22 0
11 HD 268949 sg* 05 03 13.6191878568 -68 33 35.382097584   11.83 11.76     A0Ia 24 0
12 HD 268946 sg* 05 05 12.2203060992 -66 44 12.572004624 9.86 10.41 10.42 10.28 10.17 A0Ia 54 0
13 HD 33579 sg* 05 05 55.5114721104 -67 53 10.932988848   9.32 9.13     A2Ia+ 148 0
14 HD 269070 * 05 05 58.1248247712 -70 32 05.621844336   11.70 11.061   10.147 K5 16 1
15 HD 269110 LP* 05 09 10.6083407328 -69 36 12.203504280 12.51 11.76 10.82     G0I: 38 0
16 HD 269331 s?y 05 18 01.8324453648 -69 33 37.767513132   10.56 10.31 9.72 9.869 A5Ia0 37 0
17 SK -69 99 * 05 18 30.1694226624 -69 13 14.054852460   11.76 11.94     A0I 14 0
18 SV* HV 2450 LP* 05 19 53.2668825000 -68 04 03.693824616   14.38   9.28   M1 26 0
19 SP77 48-6 LP* 05 21 46.9782726720 -71 19 43.909297248   13.4 12.0     M 16 0
20 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
21 CD-69 310 * 05 27 51.2040062256 -69 00 55.364646168 11.13 10.96 10.70     F2I 26 0
22 SK -69 148 s*y 05 28 27.9201154224 -69 12 57.413507868 14.093 12.54 10.93 10.23   G2Ia 26 0
23 HD 269604 sg* 05 28 31.3672496208 -68 53 55.749735564   10.87 10.74     A1Ia0 44 0
24 [W60] D17 s*r 05 30 02.2715021712 -67 02 45.077639712 14.883 13.05 11.29 9.21   K5I 23 0
25 HD 269651 * 05 30 32.4335586624 -69 09 11.891129364   10.92 10.73     F0I 31 0
26 HD 269661 sg* 05 30 50.0811353208 -69 31 29.399422332 9.95 10.47 10.34 10.16 10.03 A0Ia0e: 61 0
27 HD 269662 sg* 05 30 51.4749432240 -69 02 58.590657600 10.23 10.52 10.28 10.40 10.390 A0Ia 113 0
28 HD 269697 s*y 05 31 38.4223359696 -67 28 11.562011760 10.99 10.69 10.28     F6Ia 64 0
29 HD 269723 s*y 05 32 24.9642601152 -67 41 53.614053924   10.98 9.91     G4_0 62 0
30 HD 269762 sg* 05 34 09.9708489168 -68 59 12.649096680   11.45 11.37     A2Ia 28 0
31 HD 269781 sg* 05 34 22.4676706872 -67 01 23.569790196 9.34 9.94 9.87 9.74 9.67 A0Iae 64 0
32 HD 269787 sg* 05 34 34.3613333256 -66 58 23.423003256 10.58 10.99 10.73 10.73 10.71 A0Ia0 38 0
33 2MASS J05344326-6704104 * 05 34 43.2717587808 -67 04 10.462787184   13.65 11.92 11.11   ~ 9 0
34 HD 269807 sg* 05 35 00.2460003408 -67 01 12.688899816 11.13 11.01 10.85 10.89 10.662 A5Ia 35 0
35 HD 269840 s*y 05 36 10.0810875264 -68 55 41.264091912   10.74 10.334   9.774 F3Ia 45 0
36 HD 269857 sg* 05 36 32.3788464672 -68 54 01.671345252   10.64 10.29     A9Ia 50 0
37 HD 269879 s*y 05 36 47.1963137928 -66 45 46.005992280 12.87 12.02 10.94     G2Ia 39 0
38 HD 269902 sg* 05 38 09.5829719016 -69 06 21.316154364   10.59 10.23     A1Ia+ 45 0
39 HD 269953 s*y 05 40 12.1666201344 -69 40 04.853223012   10.83 9.95     G0_0 94 0
40 HD 269982 sg* 05 40 57.8100594504 -69 15 31.143653028   11.15 10.79     A3Ia 44 0
41 CPD-69 496 s*y 05 40 59.1411489120 -69 20 35.438465400   11.94 11.30     F6Ia 28 0
42 HD 270050 s*y 05 42 29.1686592048 -67 19 41.961744048   11.24 10.84     F6Ia 38 0
43 GD 71 WD* 05 52 27.6198591816 +15 53 13.228887444 11.675 12.783 13.032 13.169 13.337 DA1.5 407 0
44 * eta Hya bC* 08 43 13.4757536071 +03 23 55.182801587 3.380 4.100 4.300 4.37 4.56 B3V 418 1
45 BD+18 2910 * 14 40 45.5234393352 +17 54 07.670147040   11.47 11.47     A0 19 0
46 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 492 0
47 * rho Cas LP* 23 54 23.0325302520 +57 29 57.774737400 7.00 5.85 4.59 3.63 2.89 G2_0 401 0

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