2025A&A...697A.152K


Query : 2025A&A...697A.152K

2025A&A...697A.152K - Astronomy and Astrophysics, volume 697A152 (2025/5-1)

Variability of Galactic blue supergiants observed with TESS.

KOURNIOTIS M., CIDALE L.S., KRAUS M., RUIZ DIAZ M.A. and ALBERICI ADAM A.

Abstract (from CDS):

Context. Blue supergiants (BSGs) span phases between the main sequence and the late stages of massive stars, which makes them valuable for assessing the physics that drives stars across diverse evolutionary channels.
Aims. By exploring correlations between the parameters of BSGs and their variability properties, we aim to improve the constraints on models of the evolved star structure and on the physics of post-main-sequence evolution.
Methods. We conducted a variability study of 41 BSGs with known spectroscopic parameters in the Galaxy using high-precision photometry from the Transiting Exoplanet Survey Satellite. Stellar luminosities were calculated from the fit of multiband photometry and using the latest distance estimates from Gaia. We described the time domain of the stars by means of three statistical measures and extracted prominent frequencies via an iterative pre-whitening process. We also investigated the debated stochastic low-frequency (SLF) variability, which manifests itself in all amplitude spectra.
Results. We report a positive correlation between the amplitude of photometric variability and the stellar luminosity. For log (L/L⊙) ≲ 5, stars display frequencies that match the rotational one, suggesting that variability is driven by surface spots and/or features embedded in the wind. For log (L/L⊙) ≳ 5, variables of the α Cygni class manifest themselves via their diverse and/or time-variant photometric properties and their systematically lower frequencies. Moreover, we report a positive correlation between the SLF variability amplitude and the effective temperature, which indicates that the stellar age plays an influential role in the emergence of the background signal beyond the main sequence. A positive, though weak, correlation is also observed between the intrinsic brightness and the SLF variability amplitude, similar to the findings in the Large Magellanic Cloud, which suggests an excitation mechanism that depends only mildly on metallicity. Exceptionally, the α Cygni variables display a suppressed SLF variability that points to the interior changes that the evolving stars undergo.

Abstract Copyright: © The Authors 2025

Journal keyword(s): stars: evolution - stars: massive - stars: oscillations - stars: rotation - stars: variables: general

Status at CDS : All or part of tables of objects will not be ingested in SIMBAD.

Simbad objects: 42

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Number of rows : 42
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 LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
2 * iot CMa s*b 06 56 08.2245944314 -17 03 15.259069948 3.62 4.297 4.385 6.40   B3Ib 184 0
3 * J Pup s*b 07 53 18.1574768969 -48 06 10.566474468 3.11 4.10 4.24 4.26 4.38 B0.5Ib 249 0
4 HD 74371 s*b 08 41 56.9097314184 -45 24 38.562399648 4.94 5.378 5.227 6.75   B6Iab/b 98 0
5 HD 75149 s*b 08 46 30.5469120768 -45 54 45.019158300 5.25 5.677 5.459 6.77   B5Iab 115 0
6 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
7 HD 79186 s*b 09 11 04.3980934536 -44 52 04.448548776 4.65 5.22 5.00 4.71 4.49 B5Ia 149 0
8 HD 80558 s*b 09 18 42.3559197816 -51 33 38.338564212 6.15 6.47 5.93 5.36 4.94 B6Ia 124 0
9 * h Car * 09 34 26.6508147 -59 13 47.107031 3.58 4.09 4.09 4.00 4.01 B5II 85 0
10 HD 91619 s*b 10 33 25.3890641664 -58 11 24.536432148 6.21 6.61 6.26 5.79 5.51 B6Iab 114 0
11 HD 92964 s*b 10 42 40.5664557600 -59 12 56.730301164 5.12 5.78 5.51 5.30 5.00 B2.5Ia 155 0
12 HD 93840 s*b 10 49 08.6893503096 -46 46 41.830610088   7.71 7.79     BN1Ib 74 0
13 HD 94493 s*b 10 53 15.0996282120 -60 48 53.198014608 6.43 7.75 7.59 8.17   B0.5Iab/b 105 0
14 HD 96248 s*b 11 04 57.5664906864 -59 51 32.045356224 5.97 6.728 6.571 7.49   B1Iab 115 0
15 HD 99857 * 11 28 27.1944074808 -66 29 21.368705316 6.81 7.57 7.49 8.63   B1Ib 88 0
16 HD 99953 s*b 11 29 15.1353875280 -63 33 14.179307040 6.28 6.88 6.57 6.16 5.92 B2Ia 109 0
17 HD 103779 * 11 56 57.5476332144 -63 14 56.724069084 6.35 7.185 7.220 8.32   B0.5II 109 0
18 HD 105071 * 12 05 53.6200137672 -65 32 48.754130532 6.05 6.436 6.303     B8Ia 55 0
19 HD 106343 s*b 12 14 16.9257756576 -64 24 30.669334128 5.58 6.292 6.235     B1.5Ia 93 0
20 HD 108002 * 12 24 55.9571476872 -65 12 39.649886676 6.3 7.008 6.955 7.85   B2Ia/ab 67 0
21 HD 109867 s*b 12 38 52.3591679664 -67 11 34.979127864 5.5 6.263 6.265 7.45   B0.5/1Iab 103 0
22 HD 111558 * 12 51 11.9615376216 -69 38 42.751242564 6.92 7.38 7.25 8.16   B7Ib 50 0
23 * kap Cru SB* 12 53 48.9198156672 -60 22 34.469837436 5.62 6.12 5.94 7.12   B5I 133 0
24 HD 115842 s*b 13 20 48.3393402216 -55 48 02.482824528 5.70 6.39 6.09 5.77 5.52 B0.5Ia 162 0
25 HD 116084 * 13 22 16.2861588768 -52 10 58.631374776 5.30 6.02 5.91 5.75 5.65 B2Ib 67 0
26 HD 117024 * 13 29 05.4159397872 -63 52 26.513934384 6.44 7.126 7.109     B2Ib 46 0
27 HD 119646 s*b 13 46 17.9986132104 -62 27 05.755449348 6.03 6.674 6.620 7.49   B1.5Ib 56 0
28 HD 122879 V* 14 06 25.1578487688 -59 42 57.254187024 5.90 6.64 6.50 6.33 6.18 B0Ia 182 1
29 * v Cen * 14 20 19.5426743674 -56 23 11.383769043 4.04 4.47 4.35 4.20 4.06 B5II 91 0
30 HD 125545 * 14 22 03.0159603528 -58 17 28.374307188 6.84 8.01 7.91 8.43   B1Iab/b 38 0
31 HD 141318 Pu* 15 51 06.8041626360 -55 03 19.928655972 5.13 5.756 5.767 7.08   B2III 93 0
32 HD 142758 s*b 15 59 23.7399409248 -58 43 34.398774588 6.62 7.236 7.072 7.96   B1Ia 66 0
33 HD 148379 s*b 16 29 42.3277745448 -46 14 35.630932596 5.51 5.95 5.37 4.85 4.39 B2Iab 191 0
34 HD 148688 s*b 16 31 41.7687715992 -41 49 01.732565676 5.16 5.78 5.39 5.05 4.70 B1Iaeqp 170 0
35 * mu. Nor s*b 16 34 05.0193637737 -44 02 43.120603946 4.05 4.99 4.94 6.36   O9.7Iab 286 0
36 HD 150168 s*b 16 41 40.2261742224 -49 39 05.588433432 4.88 5.67 5.68 5.64 5.60 B1Iab/Ib 94 0
37 HD 150898 s*b 16 47 19.6583362032 -58 20 29.199122664 4.70 5.55 5.61 5.61 5.62 B0Ib 138 0
38 HD 152235 s*b 16 53 58.8528412848 -41 59 39.577848180 6.47 6.92 6.38 5.84 5.42 B0.5Ia 205 0
39 HD 152234 s*b 16 54 01.8373785611 -41 48 22.987399147 4.92 5.64 5.45     B0.5Ia 201 0
40 * k Sco s*b 17 04 49.3516568736 -34 07 22.541680380 4.44 5.13 4.87 4.59 4.42 B2Iab 158 0
41 HD 155985 * 17 17 05.5418093736 -44 46 42.944032272 6.04 6.656 6.487 7.47   B0.5Ib 69 0
42 HD 157038 s*b 17 22 39.2179927464 -37 48 16.699933296 6.99 7.20 6.44 5.70 5.15 B3Iap 115 0

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