2022A&A...659A..98S


Query : 2022A&A...659A..98S

2022A&A...659A..98S - Astronomy and Astrophysics, volume 659A, 98-98 (2022/3-1)

Detailed models of interacting short-period massive binary stars.

SEN K., LANGER N., MARCHANT P., MENON A., DE MINK S.E., SCHOOTEMEIJER A., SCHURMANN C., MAHY L., HASTINGS B., NATHANIEL K., SANA H., WANG C. and XU X.T.

Abstract (from CDS):

Context. The majority of massive stars are part of binary systems. In about a quarter of these, the companions are so close that mass transfer occurs while they undergo core hydrogen burning, first on the thermal and then on the nuclear timescale. The nuclear timescale mass transfer leads to observational counterparts: the semi-detached so-called massive Algol binaries. These systems may provide urgently needed tests of the physics of mass transfer. However, comprehensive model predictions for these systems are sparse. Aims. We use a large grid of detailed evolutionary models of short-period massive binaries and follow-up population synthesis calculations to derive probability distributions of the observable properties of massive Algols and their descendants. Methods. Our results are based on ∼10 000 binary model sequences calculated with the stellar evolution code MESA, using a metallicity suitable for the Large Magellanic Cloud (LMC), covering initial donor masses between 10 M and 40 M and initial orbital periods above 1.4 d. These models include internal differential rotation and magnetic angular momentum transport, non-conservative mass and angular momentum transfer between the binary components, and time-dependent tidal coupling. Results. Our models imply ∼30, or ∼3% of the ∼1000, core hydrogen burning O-star binaries in the LMC to be currently in the semi-detached phase. Our donor models are up to 25 times more luminous than single stars of an identical mass and effective temperature, which agrees with the observed Algols. A comparison of our models with the observed orbital periods and mass ratios implies rather conservative mass transfer in some systems, while a very inefficient one in others. This is generally well reproduced by our spin-dependent mass transfer algorithm, except for the lowest considered masses. The observations reflect the slow increase of the surface nitrogen enrichment of the donors during the semi-detached phase all the way to CNO equilibrium. We also investigate the properties of our models after core hydrogen depletion of the donor star, when these models correspond to Wolf-Rayet or helium+OB star binaries. Conclusions. A dedicated spectroscopic survey of massive Algol systems may allow to derive the dependence of the efficiency of thermal timescale mass transfer on the binary parameters, as well as the efficiency of semiconvective mixing in the stellar interior. This would be a crucial step towards reliable binary models up to the formation of supernovae and compact objects.

Abstract Copyright: © ESO 2022

Journal keyword(s): stars: massive - stars: evolution - binaries: close - stars: abundances - stars: statistics

Simbad objects: 55

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Number of rows : 55
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11146 1
2 NGC 330 Cl* 00 56 18.55 -72 27 45.1 9.37 9.76 9.55   8.89 ~ 410 0
3 V* AQ Cas EB* 01 19 10.3486523184 +62 23 48.388965936   10.84 10.31     A9 63 0
4 V* XX Cas EB* 01 29 34.6144124544 +60 58 04.706215788   9.73 9.57     B4Vn 39 0
5 V* IZ Per EB* 01 32 05.4853122768 +54 01 08.265992052   8.07 8.01     B8 80 0
6 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 164 2
7 * bet Per EB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1219 1
8 SV* HV 2241 V* 04 57 15.7351536912 -66 33 54.281614680   13.82 13.96     O6-8V-III((f)) 30 0
9 V* TT Aur EB* 05 09 42.2877371736 +39 35 10.735137888 8.65 8.668 8.602     B2Vn 137 0
10 HD 33357 Be* 05 11 42.9274371912 +42 09 55.275165324 7.67 8.55 8.55     B1:V:ne 181 0
11 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17432 0
12 SK -67 105 EB* 05 26 06.1884853848 -67 10 56.784543384 11.785 12.27 12.42   11.661 OB 39 0
13 [L72] LH 54-425 SB* 05 26 24.2505 -67 30 17.194   12.915 13.130     O3V+O5V 17 0
14 SV* HV 2543 EB* 05 27 27.3922227816 -67 11 54.502222164 11.913 13.014 13.206   13.055 OB 23 0
15 V* IU Aur SB* 05 27 52.3995663216 +34 46 58.262388600 7.91 8.55 8.37     O9.5V+B0.2V 181 0
16 W61 28-22 EB* 05 34 48.1069861728 -69 42 36.503825328   12.81 12.97 13.06 13.04 O7III 21 0
17 * tet01 Ori B EB* 05 35 16.1339860056 -05 23 06.784444248 7.71 8.20 7.96     B1V 367 2
18 [M2002] LMC 168477 SB* 05 37 30.7455556488 -69 05 17.472184188   15.49 15.35 15.30 15.28 O8.5V+O9V 13 0
19 [ST92] 1-28 LP* 05 37 37.9620597480 -69 10 14.736356688 13.515 14.211 14.161   13.713 O3.5Inf*p+sec? 15 0
20 [ST92] 1-77 SB* 05 37 50.9567494224 -69 11 00.205458504   14.81 15.0   14.570 O6V:((f))+O9.5:V: 16 0
21 Cl* NGC 2070 MEL 50 SB* 05 38 38.4788632824 -69 06 22.016378160   13.80 13.655   13.314 O9.7III:+O7:: 26 0
22 NGC 2070 Cl* 05 38 42 -69 06.0     7.25     ~ 378 1
23 [HSH95] 38 ** 05 38 42.0996 -69 06 07.795           O3V+O6V 23 0
24 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2019 2
25 MH 12 SB* 05 38 43.026 -69 04 13.15   13.96 13.99     ON9Ia:+O7.5:I:(f): 18 0
26 W61 7-14 SB* 05 38 51.0432314808 -69 06 20.499375204 13.350 14.202 13.835   13.633 B2Ip+O9III: 25 0
27 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5     O8(f)p 640 2
28 V* SV Gem EB* 06 00 41.0193040944 +24 28 25.859564076   10.98 10.57     B3 41 0
29 * del Pic EB* 06 10 17.9084822394 -54 58 07.114472168 3.55 4.49 4.72     B1/2(III)n 161 0
30 * 29 CMa SB* 07 18 40.3789353696 -24 33 31.318248528 3.80 4.80 4.95 4.95 5.08 O7Iafpvar 417 0
31 V* TU Mon EB* 07 53 19.7486798832 -03 02 31.139762712   9.21 9.24     B2-6Vn 90 0
32 V* V Pup EB* 07 58 14.4385627944 -49 14 41.694740016 3.28 4.24 4.41     B1Vp+B2: 246 0
33 HD 93206 EB* 10 44 22.9085235888 -59 59 35.970489960 5.53 6.37 6.24 7.42   O9.7Ibn 215 0
34 V* HH Car EB* 10 53 36.6688581336 -59 27 17.836206984 10.13 10.79 10.50 10.37   OB 44 0
35 V* GN Car EB* 11 08 59.7020683320 -64 19 28.090730352     12.82     ~ 6 0
36 NGC 3766 OpC 11 36 14.6 -61 36 58   5.66 5.3     ~ 213 0
37 V* BF Cen EB* 11 36 17.0350090608 -61 28 01.402061376   8.508 8.484   8.619 B8 49 0
38 V* MP Cen EB* 11 43 45.7525915968 -61 44 36.008805732 9.72 10.40 10.29 10.26 9.729 OB 36 0
39 V* BY Cru EB* 12 04 48.6318279024 -62 00 08.193672324 7.85 8.18 7.63 8.70   F0Ib/II 38 0
40 V* AI Cru EB* 12 06 07.6880185272 -61 15 24.830595468 8.93 9.67 9.69 9.43 9.26 B4/5 91 0
41 V* AB Cru EB* 12 17 37.1227102224 -58 09 52.438865868 7.75 8.59 8.49 9.53   O8III 75 0
42 HD 149404 s*b 16 36 22.5628499784 -42 51 31.902127776 5.23 5.88 5.52 6.90   O8.5Iab(f)p 249 1
43 * mu.01 Sco EB* 16 51 52.2283548696 -38 02 50.638070400 1.98 2.82 2.98     B1V+B 295 0
44 V* RZ Sct EB* 18 26 33.5232714792 -09 12 05.987275200 8.09 8.24 7.53     B2/3Ib/II 170 0
45 V* V356 Sgr EB* 18 47 52.3312296264 -20 16 28.243688340   7.07 6.99     B9III 173 0
46 V* V337 Aql EB* 19 04 10.1938278792 -02 01 47.063922312 8.58 9.315 8.890 9.51   B0.5V 68 0
47 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4337 0
48 V* V448 Cyg SB* 20 06 09.9484340064 +35 23 09.618394920 7.89 8.45 8.16     O9.5V+B1Ib 152 0
49 V* V453 Cyg EB* 20 06 34.9661707872 +35 44 26.269865844 7.83 8.52 8.40     B0.4IV+B0.7IV 206 0
50 V* V454 Cyg EB* 20 15 56.7746840424 +37 30 30.569407740   11.66 11.29     ~ 27 0
51 HD 229179 EB* 20 23 10.8281070840 +39 09 44.369496684 11.08 10.75 9.94     B1:III: 49 0
52 BD+40 4220 s*b 20 32 22.4238071594 +41 18 18.942475904 11.32 10.61 9.185     O7Iafep 399 0
53 * 14 Cep SB* 22 02 04.5726270264 +58 00 01.309758516 4.77 5.551 5.542     O9IV(n)var+B1:V: 255 0
54 V* XZ Cep EB* 22 32 25.0788763008 +67 09 02.479638996   9.22 8.51     O9.5V 99 0
55 V* GT Cep EB* 22 57 47.3140536144 +68 24 26.036646516   8.49 8.25     B5II 71 0

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