2025A&A...704A.219S


Query : 2025A&A...704A.219S

2025A&A...704A.219S - Astronomy and Astrophysics, volume 704A219 (2025/12-1)

Populations of evolved massive binary stars in the Small Magellanic Cloud II. Predictions from rapid binary evolution.

SCHURMANN C., XU X.-T., LANGER N., LENNON D., KRUCKOW M.U., ANTONIADIS J., HABERL F., HERRERO A., KRAMER M., SCHOOTEMEIJER A., SHENAR T., TAURIS T.M. and WANG C.

Abstract (from CDS):

Context. Massive star evolution plays a crucial role in astrophysics; however, its study is subject to large uncertainties. This problem becomes more severe by the majority of massive stars being born in close binary systems, whose evolution is affected by interactions among their components.
Aims. We want to constrain major uncertainties in massive binary star evolution, particularly with respect to the efficiency and the stability of the first mass-transfer phase.
Methods. We used the rapid population synthesis code COMBINE to generate synthetic populations of post-interaction binaries, assuming constant mass-transfer efficiency. We employed a new merger criterion that adjusts self-consistently to any prescribed mass-transfer efficiency. We tailored our synthetic populations to be comparable to the expected binary populations in the Small Magellanic Cloud (SMC).
Results. We find that the observed populations of evolved massive binaries cannot be reproduced with a single mass-transfer efficiency. Instead, a rather high efficiency (≳50%) is needed to reproduce the number of Be stars and Be/X-ray (BeXB) binaries in the SMC, while a low efficiency (∼10%) leads to a better agreement with the observed number of Wolf-Rayet (WR) stars. We constructed a corresponding mass-dependent mass-transfer efficiency recipe to produce our fiducial synthetic SMC post-interaction binary population. It reproduces the observed number and properties of the BeXBs and WR binaries rather well; furthermore, it is not in stark disagreement with the observed OBe star population. It predicts around 170 massive stars with neutron star companion, of which 140 are Be stars, and about 170 systems disrupted by the supernova, of which 150 are Be stars. Overall, 20% of all post-interaction systems contain a helium star. It also predicts two large, as-yet-unobserved populations of OB + BH binaries: about 100 OB + BH systems with rather small orbital periods (≲20 d) and around 40 longer period OBe + BH systems.
Conclusions. Continued searches for massive binary systems will strongly advance our understanding of their evolution.

Abstract Copyright: © The Authors 2025

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

Simbad objects: 26

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Number of rows : 26
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 PSR J0045-7319 HXB 00 45 35.2606875816 -73 19 03.269105220   15.97 16.18   16.30 B0.5-B2IV-V 193 0
2 LIN 143 WR* 00 49 59.3505485400 -73 22 14.121279948 13.48 14.43 14.56   14.57 WN3/4+O4 45 0
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 419 1
5 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
6 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
7 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
8 LIN 547 WR* 01 31 04.1367366432 -73 25 03.784411524   12.75 12.90     WO4+O4V 104 0
9 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 187 2
10 * alf Eri Be* 01 37 42.84548 -57 14 12.3101 -0.36 0.30 0.46 0.49 0.60 B6Vpe 495 1
11 * phi Per Be* 01 43 39.6379691568 +50 41 19.433124998 3.10 4.02 4.06 3.90 3.88 B1.5V:e-shell 594 0
12 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
13 * bet Per SB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1265 1
14 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
15 1A 0535-668 HXB 05 35 40.9970566152 -66 51 53.547559416       15.036 15.138 B2IIIe 302 0
16 2MASS J05380840-6909190 SB* 05 38 08.4066684408 -69 09 18.975749724   15.47 15.26     O7V(n)((f)) 44 0
17 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
18 LS V +22 25 Be* 06 11 49.0761116160 +22 49 32.686712760 11.5 11.788 11.468 11.451   B3V 96 0
19 Mrk 116 AGN 09 34 02.1 +55 14 25           ~ 1179 1
20 * alf Leo PM* 10 08 22.31099 +11 58 01.9516 0.88 1.24 1.40 1.37 1.47 B8IVn 891 1
21 * del Lib SB* 15 00 58.3483018872 -08 31 08.210408772 4.82 4.93 4.93 4.85 4.84 A0V 305 0
22 * zet Oph Be* 16 37 09.5400587698 -10 34 01.509742704 1.73 2.58 2.56 2.46 2.50 O9.2IVnn 1908 0
23 * bet Lyr SB* 18 50 04.7951442356 +33 21 45.600371200 2.85 3.42 3.42 3.31 3.29 B8.5Ib-II 955 0
24 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
25 Ass Cyg OB 2 As* 20 33.2 +41 19           ~ 1023 0
26 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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