2024A&A...690A.126H


Query : 2024A&A...690A.126H

2024A&A...690A.126H - Astronomy and Astrophysics, volume 690A126 (2024/10-1)

Empirical mass-loss rates and clumping properties of O-type stars in the Large Magellanic Cloud.

HAWCROFT C., MAHY L., SANA H., SUNDQVIST J.O., ABDUL-MASIH M., BRANDS S.A., DECIN L., DE KOTER A. and PULS J.

Abstract (from CDS):

Context. The nature of mass-loss in massive stars is one of the most important and difficult to constrain processes in the evolution of massive stars. The largest observational uncertainties are related to the influence of metallicity and wind structure with optically thick clumps.
Aims. We aim to constrain the wind parameters of sample of 18 O-type stars in the LMC, through analysis with stellar atmosphere and wind models including the effects of optically thick clumping. This will allow us to determine the most accurate spectroscopic mass-loss and wind structure properties of massive stars at sub-solar metallicity to date. This will allow us to gain insight into the impact of metallicity on massive stellar winds.
Methods. Combining high signal to noise (S/N) ratio observations in the ultraviolet and optical wavelength ranges gives us access to diagnostics of multiple different ongoing physical processes in the stellar wind. We produce synthetic spectra using the stellar atmosphere modelling code FASTWIND, and reproduce the observed spectra using a genetic algorithm based fitting technique to optimise the input parameters.
Results. We empirically constrain 15 physical parameters associated with the stellar and wind properties of O-type stars from the dwarf, giant and supergiant luminosity classes. These include temperature, surface gravity, surface abundances, rotation, macroturbulence and wind parameters.
Conclusions. We find, on average, mass-loss rates a factor of 4-5 lower than those from theoretical predictions commonly used in stellar-evolution calculations, but in good agreement with more recent theoretical predictions. In the 'weak-wind' regime we find massloss rates orders of magnitude below any theoretical predictions. We find a positive correlation of clumping factors with effective temperature with an average fcl = 14 ± 8 for the full sample. It is clear that there is a difference in the porosity of the wind in velocity space, and interclump density, above and below a temperature of roughly 38 kK. Above 38 kK an average 46 ± 24% of the wind velocity span is covered by clumps and the interclump density is 10-30% of the mean wind. Below an effective temperature of roughly 38 kK there must be additional light leakage for supergiants. For dwarf stars at low temperatures there is a statistical preference for very low clump velocity spans, however it is unclear if this can be physically motivated as there are no clearly observable wind signatures in UV diagnostics.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: atmospheres - stars: early-type - stars: fundamental parameters - stars: massive - stars: mass-loss - stars: winds, outflows

Simbad objects: 21

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Number of rows : 21
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 SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 2MASS J05373664-6907318 s*b 05 37 36.6560452584 -69 07 31.823879304   13.44 13.58     O9.7Ib-II 16 0
4 2MASS J05373854-6910199 SB* 05 37 38.5076245200 -69 10 19.862759784 12.875 13.744 13.710   13.555 O6V((n))((fc))z 13 0
5 [ST92] 1-60 SB* 05 37 45.4999 -69 11 09.507   15.55 15.6     O3.5V((fc)) 7 0
6 Brey 74a WR* 05 37 51.3386549880 -69 09 46.690186716 12.483 13.474 13.446 13.62 13.278 O3If* 43 0
7 2MASS J05375180-6904248 SB* 05 37 51.8212746648 -69 04 24.742740252   15.29 15.38     O6.5Vnz 8 0
8 UCAC2 1803316 * 05 37 59.0526663864 -69 11 56.710162752 13.935 14.655 14.389 14.49 14.035 O4V((fc)) 14 0
9 NAME 30 Dor Region reg 05 38.0 -69 06           ~ 261 0
10 UCAC2 1803324 SB* 05 38 00.6042085320 -69 08 41.807071032   14.72 14.8 15.15   O9.5IV 12 0
11 VFTS 235 * 05 38 06.3511926552 -69 05 14.263478160   15.42 15.48     O9.7III 9 0
12 2MASS J05380840-6905446 SB* 05 38 08.4091730688 -69 05 44.487386376   13.94 14.04     O5III(n)(fc) 13 0
13 VFTS 280 * 05 38 16.5491532984 -69 04 53.193397620   15.4 15.40     O9V((n)) 11 0
14 Cl* NGC 2070 SMB 84 SB* 05 38 32.34 -69 05 23.7   14.65 14.65   14.79 O4-5V((n))((fc)) 18 0
15 Cl* NGC 2070 SMB 140 SB* 05 38 35.9954763336 -69 06 16.948926828   15.38 15.14   14.58 O4III(f) 11 0
16 Cl* NGC 2070 MEL 47 SB* 05 38 37.718 -69 05 20.97 11.913 12.764 12.046   12.344 O6-6.5II(f) 24 0
17 Cl* NGC 2070 MEL 29 * 05 38 41.9333563008 -69 04 38.813563056   14.64 14.72   14.467 O9.5V-III((n)) 13 0
18 2MASS J05384539-6902514 pA? 05 38 45.3901880400 -69 02 51.448462044 13.564 14.574 14.491 13.97 14.826 O4V((n))((fc))z 24 0
19 Cl* NGC 2070 MH 999 SB* 05 38 46.7865227544 -69 06 03.188070828   14.38 14.22   14.03 O4III(f) 27 0
20 [P93] 9034 * 05 38 48.4032393744 -68 59 49.916028984 14.379 15.246 15.339   15.591 O9.7V 14 0
21 W61 7-19 * 05 38 52.7246801448 -69 06 43.267945464 13.481 14.132 13.937   13.702 O7II(f) 26 0

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