2025A&A...704A.218X


Query : 2025A&A...704A.218X

2025A&A...704A.218X - Astronomy and Astrophysics, volume 704A218 (2025/12-1)

Populations of evolved massive binary stars in the Small Magellanic Cloud I. Predictions from detailed evolution models.

XU X.-T., SCHURMANN C., LANGER N., WANG C., SCHOOTEMEIJER A., SHENAR T., ERCOLINO A., HABERL F., HASTINGS B., JIN H., KRAMER M., LENNON D., MARCHANT P., SEN K., TAURIS T.M. and DE MINK S.E.

Abstract (from CDS):

Context. The majority of massive stars are born with a close binary companion. How this affects their evolution and fate is still largely uncertain, especially at low metallicity.
Aims. We derive synthetic populations of massive post-interaction binary products and compare them with corresponding observed populations in the Small Magellanic Cloud (SMC).
Methods. We analyse 53298 detailed binary evolutionary models computed with MESA. Our models include the physics of rotation, mass and angular momentum transfer, magnetic internal angular momentum transport, and tidal spin-orbit coupling. They cover initial primary masses of 5-100 M⊙, initial mass ratios of 0.3-0.95, and all initial periods for which interaction is expected, 1-3162 d. They are evolved through the first mass transfer and the donor star death, and a a possible ensuing Be X-ray binary phase, and they end when the mass gainer leaves the main sequence.
Results. In our fiducial synthetic population, 8% of the OB stars in the SMC are post-mass-transfer systems, and 7% are merger products. In many of our models, the mass gainers are spun up and expected to form Oe/Be stars. While our model underpredicts the number of Be X-ray binaries in the SMC, it reproduces the main features of their orbital period distribution and the observed number of SMC binary WR stars. We further expect ∼50 OB+BH binaries below and ∼170 above the 20 d orbital period. The long-period OB+BH binaries might produce merging double black holes. However, their progenitors, the predicted long-period WR+OB binaries, are not observed.
Conlcusions. While the comparison with the observed SMC stars supports many physics assumptions in our high-mass binary models, a better match for the large number of observed OBe stars and Be X-ray binaries likely requires a lower merger rate and/or a higher mass transfer efficiency during the first mass transfer. The fate of the initially wide O star binaries remains particularly uncertain.

Abstract Copyright: © The Authors 2025

Journal keyword(s): stars: black holes - stars: emission-line, Be - stars: neutron - stars: Wolf-Rayet - Magellanic Clouds - X-rays: binaries

Simbad objects: 23

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Number of rows : 23
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 SMC AB 1 WR* 00 43 42.3082596960 -73 28 55.259220360 14.33 15.20 15.24   15.21 WN3+O4: 37 0
2 PSR J0045-7319 HXB 00 45 35.2606875816 -73 19 03.269105220   15.97 16.18   16.30 B0.5-B2IV-V 193 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 57 0
4 LIN 143 WR* 00 49 59.3505485400 -73 22 14.121279948 13.48 14.43 14.56   14.57 WN3/4+O4 45 0
5 LIN 160 WR* 00 50 43.4248908624 -73 27 05.815089828 12.363 13.304 13.426   13.55 WN6 58 0
6 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
7 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 419 1
8 RMC 31 WR* 01 03 25.2272050176 -72 06 43.857668340   12.11 12.30     WN3:h+O5.5V+O5.5If+O7.5V 126 0
9 SMC AB 7 WR* 01 03 35.9241336168 -72 03 22.118601312 11.933 12.954 13.016   13.32 WN4+O6I(f) 58 0
10 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
11 LIN 547 WR* 01 31 04.1367366432 -73 25 03.784411524   12.75 12.90     WO4+O4V 104 0
12 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 187 2
13 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
14 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
15 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
16 1A 0535-668 HXB 05 35 40.9970566152 -66 51 53.547559416       15.036 15.138 B2IIIe 302 0
17 2MASS J05380840-6909190 SB* 05 38 08.4066684408 -69 09 18.975749724   15.47 15.26     O7V(n)((f)) 44 0
18 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
19 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
20 HD 130298 SB* 14 49 33.7650740400 -56 25 38.474619060 9.14 10.06 9.83 9.65   O6.5III(n)(f) 90 0
21 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
22 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
23 HD 215227 HXB 22 42 57.3031579265 +44 43 18.259103226 8.07 8.84 8.78     B1.5-2III 157 0

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