2024A&A...692A..49B


Query : 2024A&A...692A..49B

2024A&A...692A..49B - Astronomy and Astrophysics, volume 692A49 (2024/12-1)

Photometric detection of internal gravity waves in upper main-sequence stars IV. Comparable stochastic low-frequency variability in SMC, LMC, and Galactic massive stars.

BOWMAN D.M., VAN DAELE P., MICHIELSEN M. and VAN REETH T.

Abstract (from CDS):

Context. Massive main-sequence stars have convective cores and radiative envelopes, but can also have sub-surface convection zones caused by partial ionisation zones. However, the convective properties of such regions strongly depend on opacity and therefore a star's metallicity. Non-rotating 1D evolution models of main-sequence stars between 7 ≤ M ≤ 40 M⊙ and the metallicity of the Small Magellanic Cloud (SMC) galaxy suggest tenuous (if any) sub-surface convection zones when using the Rayleigh number as a criterion for convection owing to their substantially lower metallicity compared to Galactic massive stars.
Aims. We test whether massive stars of different metallicities both inside and outside of asteroseismically calibrated stability windows for sub-surface convection exhibit different properties in stochastic low-frequency (SLF) variability. Thus, we aim to constrain the metallicity dependence of the physical mechanism responsible for SLF variability commonly found in light curves of massive stars.
Methods. We extracted customised light curves from the ongoing NASA Transiting Exoplanet Survey Satellite (TESS) mission for a sample of massive stars using an effective point spread function (ePSF) method, and compared their morphologies in terms of characteristic frequency, νchar, and amplitude using a Gaussian process (GP) regression methodology.
Results. We demonstrate that the properties of SLF variability observed in time series photometry of massive stars are generally consistent across the metallicity range from the Milky Way down to the SMC galaxy, for stars both inside and outside of the sub-surface stability windows based on the Rayleigh number as a criterion for convection.
Conclusions. We conclude that non-rotating 1D stellar structure models of sub-surface convection cannot alone be used to explain the mechanism giving rise to SLF variability in light curves of massive stars. Additionally, the similar properties of SLF variability across a wide range of metallicity values, which follow the same trends in mass and age in the Hertzsprung-Russell (HR) diagram at both high and low metallicity, support a transition in the dominant mechanism causing SLF variability from younger to more evolved stars. Specifically, core-excited internal gravity waves (IGWs) are favoured for younger stars lacking sub-surface convection zones, especially at low metallicity, and sub-surface convection zones are favoured for more evolved massive stars.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: early-type - stars: fundamental parameters - stars: massive - stars: oscillations - stars: rotation

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 2dFS 163 s*b 00 36 58.2381836400 -73 23 33.167140224 13.84 14.95 15.11   15.14 O7.5Ib(f) 12 0
2 LHA 115-S 6 s*b 00 46 55.0295765376 -73 08 34.136808252 12.14 13.02 12.91   12.52 BI[e] 100 1
3 SK 13 s*b 00 47 12.2164410744 -73 06 33.111710784   12.52 12.48     B1.5Ia 83 0
4 AzV 83 s*b 00 50 52.0015192368 -72 42 14.940550980 12.233 13.244 13.366   13.67 O7Iaf 58 0
5 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
6 Cl* NGC 346 MPG 12 * 00 58 14.0865065520 -72 10 44.292892764   19.15 17.98   16.72 B0III 43 0
7 AzV 202 s*b 00 58 14.4693679440 -72 07 29.549446932 13.12 14.18 14.34   14.52 B1Ib 17 0
8 NGC 346 Cl* 00 59 04.4000 -72 10 39.000           ~ 547 0
9 Cl* NGC 346 ELS 22 * 00 59 18.6176208672 -72 11 09.887619084   14.65 14.91     O9V 23 0
10 Cl* NGC 346 ELS 46 Y*O 00 59 31.8683861040 -72 13 35.225231592   15.16 15.44     O6.5Vnn 18 0
11 Cl* NGC 346 ELS 25 * 00 59 52.9567285440 -72 10 49.136185452 13.62 14.72 14.90   15.20 O9.2V 13 0
12 AzV 251 * 01 00 22.1535867240 -72 30 48.733765308 13.38 14.47 14.69   14.93 O8Vnn 23 0
13 SK 94 s*b 01 01 07.7622056304 -71 59 58.783358472   12.21 12.36 12.20   B1Ia 39 0
14 AzV 267 * 01 01 15.6926628168 -72 06 35.367953616   14.58 14.84     O7.5Vn 25 0
15 SK 116 s*b 01 04 55.7398901040 -72 46 48.146591280 11.413 12.494 12.646     O9.2Iab 43 0
16 AzV 429 EB* 01 07 59.8335369624 -72 00 53.979262812 13.40 14.49 14.69   14.91 O7Vz 23 0
17 SK 143 s*b 01 10 55.7567270880 -72 42 56.223094032 12.15 12.98 12.89 12.78 11.64 O9.7Ib 91 0
18 AzV 461 * 01 11 25.5705843312 -72 09 48.802253292 13.22 14.40 14.61   14.94 O8V+neb 25 0
19 AzV 468 * 01 12 05.8755103152 -72 40 56.600864328 13.83 14.86 15.14   15.49 O8.5V 21 0
20 SK 150 s*b 01 13 01.8742585512 -72 45 48.441989592 11.593 12.564 12.676   11.42 B1.5Ia 41 0
21 SK 155 s*b 01 14 50.2614192144 -73 20 17.851206156 11.35 12.33 12.48     O9Iab(ff) 63 0
22 SK 159 s*b 01 15 58.8782034384 -73 21 24.351532740 10.80 11.77 11.90     B0.2Ia 84 0
23 2MASS J01242798-7314150 * 01 24 27.9810601704 -73 14 14.936993232   13.77 13.97     O9.7V: 6 0
24 2dFS 3780 * 01 26 35.2855868400 -73 15 16.280587908   14.12 14.37     O9.5III 15 0
25 2dFS 3954 * 01 30 43.1041712424 -73 25 04.123554384   15.07 15.25     O7V 9 0
26 SK -66 18 Pu* 04 55 59.8226723496 -65 58 29.732367612 12.394 13.294 13.467   13.725 O6.5III((f)) 22 0
27 [L72] LH 9-89 * 04 56 11.0176066200 -66 28 24.363611436 12.580 13.531 13.645   13.837 B0IIIn 16 0
28 [ELS2006] N11 051 Pu* 04 56 29.6988034392 -66 21 38.860019604 12.909 13.812 13.990   14.173 O5Vn((f)) 14 0
29 [ELS2006] N11 046 * 04 56 44.6245232208 -66 34 20.862623244 12.874 13.850 13.856   14.109 O9.5V 11 0
30 HD 270952 WR* 05 01 23.0763876936 -65 52 33.206008764 10.944 11.871 12.07   12.187 O6Iaf 61 0
31 SK -68 41 * 05 05 27.1146438696 -68 10 02.642123460 10.855 11.868 12.01   12.086 B0.7Ia 59 0
32 HD 269050 s*b 05 07 20.4218668824 -68 32 08.569322196 10.593 11.581 11.54 11.46 11.55 B0Ia(e?) 89 0
33 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
34 BI 173 * 05 27 09.9440507208 -69 07 56.452079568 11.85 12.86 13.00     O7.5III((f))p 36 0
35 SK -66 100 * 05 27 45.4472444328 -66 55 15.293259480 12.227 12.976 13.204   13.501 O6II(f) 48 0
36 SK -71 35 Em* 05 30 04.1770770096 -71 07 56.243598564 12.009 12.94 13.01 13.35 13.038 B1II 22 0
37 SK -71 41 s*b 05 30 40.1497148784 -71 05 37.084358652 11.906 12.643 12.775   12.769 O9.7Iab 23 0
38 RMC 109 s*b 05 30 40.4069468208 -67 16 08.942376000   12.19 12.59 11.98 12.06 B5Ia 24 0
39 HD 269698 s*b 05 31 44.2080798984 -67 38 01.374839556 9.520 12.00 12.22 12.47 11.167 O4Ia 117 0
40 W61 28-5 * 05 34 28.4650523832 -69 43 56.833403844 12.795 13.630 13.774   14.063 O4V(f+) 17 0
41 BI 237 * 05 36 14.6333257920 -67 39 19.168082640 12.865 13.790 13.830   13.948 O2V(f*) 47 0
42 HD 269889 Pu* 05 37 02.4204862512 -66 38 37.031705268 11.381 10.246 12.19   11.390 O9Ia 29 0
43 BI 253 * 05 37 34.4595697440 -69 01 10.178659452 12.765 13.650 13.669   13.742 O2V(f*) 60 0
44 HD 269896 s*b 05 37 49.1356176384 -68 55 01.639049016 11.338 9.493 11.449 11.49   ON9.7Ia+ 102 0
45 2MASS J05380840-6905446 SB* 05 38 08.4091730688 -69 05 44.487386376   13.94 14.04     O5III(n)(fc) 13 0
46 2MASS J05382913-6857393 SB* 05 38 29.1463260480 -68 57 39.327666624   13.93 14.12     O4V((n))((fc))z 14 0
47 SK -68 140 s*b 05 38 57.1713887928 -68 56 53.151615708   12.81 12.71 12.89   B0.7Ib-IabNwk 53 0

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