2016A&A...591A..22S


Query : 2016A&A...591A..22S

2016A&A...591A..22S - Astronomy and Astrophysics, volume 591A, 22-22 (2016/7-1)

Wolf-Rayet stars in the Small Magellanic Cloud. II. Analysis of the binaries.

SHENAR T., HAINICH R., TODT H., SANDER A., HAMANN W.-R., MOFFAT A.F.J., ELDRIDGE J.J., PABLO H., OSKINOVA L.M. and RICHARDSON N.D.

Abstract (from CDS):

Context. Massive Wolf-Rayet (WR) stars are evolved massive stars (Mi>=20M) characterized by strong mass-loss. Hypothetically, they can form either as single stars or as mass donors in close binaries. About 40% of all known WR stars are confirmed binaries, raising the question as to the impact of binarity on the WR population. Studying WR binaries is crucial in this context, and furthermore enable one to reliably derive the elusive masses of their components, making them indispensable for the study of massive stars.
Aims. By performing a spectral analysis of all multiple WR systems in the Small Magellanic Cloud (SMC), we obtain the full set of stellar parameters for each individual component. Mass-luminosity relations are tested, and the importance of the binary evolution channel is assessed.
Methods. The spectral analysis is performed with the Potsdam Wolf-Rayet (PoWR) model atmosphere code by superimposing model spectra that correspond to each component. Evolutionary channels are constrained using the Binary Population and Spectral Synthesis (BPASS) evolution tool.
Results. Significant hydrogen mass fractions (0.1<XH<0.4) are detected in all WN components. A comparison with mass-luminosity relations and evolutionary tracks implies that the majority of the WR stars in our sample are not chemically homogeneous. The WR component in the binary AB 6 is found to be very luminous (logL≃6.3[L]) given its orbital mass (≃10M), presumably because of observational contamination by a third component. Evolutionary paths derived for our objects suggest that Roche lobe overflow had occurred in most systems, affecting their evolution. However, the implied initial masses (>=60M) are large enough for the primaries to have entered the WR phase, regardless of binary interaction.
Conclusions. Together with the results for the putatively single SMC WR stars, our study suggests that the binary evolution channel does not dominate the formation of WR stars at SMC metallicity.

Abstract Copyright: © ESO, 2016

Journal keyword(s): stars: massive - stars: Wolf-Rayet - stars: evolution - binaries: close - binaries: symbiotic - Magellanic Clouds

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SMC AB 1 WR* 00 43 42.3082596960 -73 28 55.259220360 14.33 15.20 15.24   15.21 WN3+O4: 31 0
2 SMC AB 10 WR* 00 45 28.9085871312 -73 04 45.621712056 14.69 15.81 15.55   15.96 WN3ha 22 0
3 SMC AB 2 WR* 00 48 30.8447640360 -73 15 45.829848132 13.23 14.23 14.43   14.52 WN4.5/O3 49 0
4 LIN 143 WR* 00 49 59.3505485400 -73 22 14.121279948 13.48 14.43 14.56   14.57 WN3/4+O4 37 0
5 CXOU J004959.4-732211 X 00 49 59.4 -73 22 11           ~ 1 0
6 LIN 160 WR* 00 50 43.4248908624 -73 27 05.815089828 12.363 13.304 13.426   13.55 WN6 49 0
7 SMC AB 11 WR* 00 52 07.39 -72 35 38.6   15.593 15.816   16.011 WN4h:a 23 0
8 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11145 1
9 SMC AB 9 WR* 00 54 32.1559137576 -72 44 35.666609568 14.31 15.26 15.43   15.69 WN3ha 28 0
10 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 393 1
11 SMC AB 12 WR* 01 02 52.4011237800 -72 06 52.532688348   16 16.08     WN3ha 21 0
12 RMC 31 WR* 01 03 25.2272050176 -72 06 43.857668340   12.11 12.30     WN3:h+O5.5V+O5.5If+O7.5V 114 0
13 SMC AB 7 WR* 01 03 35.9241336168 -72 03 22.118601312 11.933 12.954 13.016   13.32 WN4+O6I(f) 48 0
14 LIN 547 WR* 01 31 04.1367366432 -73 25 03.784411524   12.75 12.90     WO4+O4V 96 0
15 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7062 0
16 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17428 0
17 [MS70] 4 WR* 10 51 38.9063499504 -60 56 34.909328328 13.57 13.80 12.78 12.56   WO4+O5III/V((f)) 52 0

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