2022A&A...663A..36B


Query : 2022A&A...663A..36B

2022A&A...663A..36B - Astronomy and Astrophysics, volume 663A36-36 (2022/7-1)

The R136 star cluster dissected with Hubble Space Telescope/STIS. III. The most massive stars and their clumped winds.

BRANDS S.A., DE KOTER A., BESTENLEHNER J.M., CROWTHER P.A., SUNDQVIST J.O., PULS J., CABALLERO-NIEVES S.M., ABDUL-MASIH M., DRIESSEN F.A., GARCIA M., GEEN S., GRAFENER G., HAWCROFT C., KAPER L., KESZTHELYI Z., LANGER N., SANA H., SCHNEIDER F.R.N., SHENAR T. and VINK J.S.

Abstract (from CDS):


Context. The star cluster R136 inside the Large Magellanic Cloud hosts a rich population of massive stars, including the most massive stars known. The strong stellar winds of these very luminous stars impact their evolution and the surrounding environment. We currently lack detailed knowledge of the wind structure that is needed to quantify this impact.
Aims. Our goal is to observationally constrain the stellar and wind properties of the massive stars in R136, in particular the wind-structure parameters related to wind clumping.
Methods. We simultaneously analyse optical and ultraviolet spectroscopy of 53 O-type and three WNh-stars using the FASTWIND model atmosphere code and a genetic algorithm. The models account for optically thick clumps and effects related to porosity and velocity-porosity, as well as a non-void interclump medium.
Results. We obtain stellar parameters, surface abundances, mass-loss rates, terminal velocities, and clumping characteristics and compare them to theoretical predictions and evolutionary models. The clumping properties include the density of the interclump medium and the velocity-porosity of the wind. For the first time, these characteristics are systematically measured for a wide range of effective temperatures and luminosities.
Conclusions. We confirm a cluster age of 1.0-2.5 Myr and derived an initial stellar mass of ≳250 M☉ for the most massive star in our sample, R136a1. The winds of our sample stars are highly clumped, with an average clumping factor of fcl = 29 ± 15. We find tentative trends in the wind-structure parameters as a function of the mass-loss rate, suggesting that the winds of stars with higher mass-loss rates are less clumped. We compare several theoretical predictions to the observed mass-loss rates and terminal velocities and find that none satisfactorily reproduce both quantities. The prescription of Krticka & Kubat (2018) matches the observed mass-loss rates best.

Abstract Copyright: © ESO 2022

Journal keyword(s): stars: massive - stars: mass-loss - stars: winds - outflows - stars: fundamental parameters - Magellanic Clouds - galaxies: star clusters: individual: R136

VizieR on-line data: <Available at CDS (J/A+A/663/A36): sources.dat tablea1.dat tablea2.dat tablei1.dat tablei2.dat>

Simbad objects: 62

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Number of rows : 62
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 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 NAME 30 Dor Nebula SFR 05 38 36.0 -69 05 11           ~ 1276 2
4 [HSH95] 120 * 05 38 41.945 -69 06 04.95           ~ 4 0
5 [HSH95] 123 * 05 38 42.065 -69 06 04.46           ~ 4 0
6 [HSH95] 162 * 05 38 42.144 -69 06 03.86           ~ 2 0
7 [HSH95] 108 * 05 38 42.184 -69 06 01.83           ~ 4 0
8 [HSH95] 134 * 05 38 42.190 -69 06 04.77           ~ 4 0
9 [HSH95] 139 * 05 38 42.199 -69 06 04.06           ~ 4 0
10 [HSH95] 75 * 05 38 42.203 -69 06 01.73           ~ 3 0
11 [HSH95] 78 * 05 38 42.222 -69 06 02.97           ~ 4 0
12 [HSH95] 90 * 05 38 42.259 -69 06 02.74           ~ 8 0
13 [HSH95] 116 * 05 38 42.270 -69 06 04.48           ~ 3 0
14 [HSH95] 92 * 05 38 42.278 -69 06 02.05           O3V 9 0
15 [HSH95] 35 * 05 38 42.281 -69 06 02.26     14.42     O3V 11 0
16 Cl* NGC 2070 MH 454 * 05 38 42.294 -69 06 03.29   14.06       ~ 19 0
17 [HSH95] 132 * 05 38 42.301 -69 06 01.51           ~ 3 0
18 [HSH95] 173 * 05 38 42.316 -69 06 01.41           ~ 3 0
19 [HSH95] 86 * 05 38 42.325 -69 06 03.06           ~ 3 0
20 [HSH95] 121 * 05 38 42.330 -69 06 04.82           ~ 3 0
21 BAT99 106 WR* 05 38 42.338 -69 06 03.21   12.83 12.93     WN5h 74 0
22 [HSH95] 30 * 05 38 42.339 -69 06 02.33     14.26     O3V 10 0
23 [HSH95] 80 * 05 38 42.343 -69 06 03.66           ~ 4 0
24 Cl* NGC 2070 MH 474 * 05 38 42.346 -69 06 02.55   13.56       ~ 18 0
25 Cl* NGC 2070 MH 480 * 05 38 42.362 -69 06 02.54   14.28       ~ 13 0
26 [HSH95] 49 * 05 38 42.371 -69 06 01.22     14.74     O3V 9 0
27 [HSH95] 159 * 05 38 42.372 -69 06 04.15           ~ 3 0
28 [HSH95] 62 * 05 38 42.381 -69 06 03.49     14.96     ~ 10 0
29 [HSH95] 71 * 05 38 42.390 -69 06 04.82     15.17     ~ 9 0
30 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
31 BAT99 108 WR* 05 38 42.396 -69 06 02.87   12.78 12.77     WN5h 99 0
32 [HSH95] 141 * 05 38 42.399 -69 06 03.61           ~ 3 0
33 Cl* NGC 2070 MH 509 * 05 38 42.414 -69 06 02.52   13.78 13.73     O3III 23 0
34 BAT99 109 WR* 05 38 42.415 -69 06 02.81   13.09 13.38     WN5h 58 0
35 [HSH95] 114 * 05 38 42.425 -69 06 04.37           ~ 4 0
36 [HSH95] 66 * 05 38 42.431 -69 06 03.29     15.13     O3V 11 0
37 [HSH95] 52 * 05 38 42.432 -69 06 03.94     14.76     O3V 11 0
38 BAT99 110 WR* 05 38 42.436 -69 06 02.67   13.73 13.73     O2If* 46 0
39 [HSH95] 135 * 05 38 42.440 -69 06 01.82           ~ 3 0
40 [HSH95] 70 * 05 38 42.465 -69 06 02.36           ~ 3 0
41 Cl* NGC 2070 MH 535 * 05 38 42.470 -69 06 01.14   14.33 14.49     O2-3.5V 21 0
42 [HSH95] 31 * 05 38 42.484 -69 06 04.37     14.35     ~ 11 0
43 [HSH95] 58 * 05 38 42.488 -69 06 02.56     14.82     O3III 12 0
44 Cl* NGC 2070 MH 551 * 05 38 42.512 -69 06 04.52   14.64 14.81     O3V 18 0
45 [HSH95] 50 * 05 38 42.514 -69 06 03.21     14.75     ~ 10 0
46 [HSH95] 112 * 05 38 42.535 -69 06 02.14           O8.5III 8 0
47 [HSH95] 94 * 05 38 42.540 -69 06 03.86           O3V 9 0
48 [HSH95] 69 * 05 38 42.549 -69 06 03.53     15.16     ~ 9 0
49 [HSH95] 73 * 05 38 42.554 -69 06 03.36           O9V 8 0
50 [HSH95] 143 * 05 38 42.587 -69 06 02.85           ~ 3 0
51 [HSH95] 48 * 05 38 42.617 -69 06 02.77     14.72     O3III 12 0
52 Cl* NGC 2070 MH 602 * 05 38 42.647 -69 06 01.80   14.67 14.63     O3III 18 0
53 [HSH95] 64 * 05 38 42.649 -69 06 00.89     15.06     O7V 11 0
54 Cl* NGC 2070 MH 608 * 05 38 42.671 -69 06 02.76   14.49 14.39     ~ 20 0
55 [HSH95] 46 * 05 38 42.699 -69 06 02.43     14.67     ~ 10 0
56 BAT99 111 WR* 05 38 42.745 -69 06 03.70   13.51 13.66     WN9ha 54 0
57 [HSH95] 65 * 05 38 42.803 -69 06 03.23     15.12     ~ 9 0
58 [HSH95] 45 * 05 38 42.836 -69 06 03.21     14.62     O3V 10 0
59 [HSH95] 129 * 05 38 43.025 -69 06 00.96           ~ 3 0
60 [HSH95] 68 * 05 38 43.200 -69 06 01.62     15.16     O3V 10 0
61 RMC 136a Cl* 05 38 43.3 -69 06 08           ~ 158 2
62 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 792 0

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