2018A&A...609A..94H


Query : 2018A&A...609A..94H

2018A&A...609A..94H - Astronomy and Astrophysics, volume 609A94-94 (2018/1-1)

Observational properties of massive black hole binary progenitors.

HAINICH R., OSKINOVA L.M., SHENAR T., MARCHANT P., ELDRIDGE J.J., SANDER A.A.C., HAMANN W.-R., LANGER N. and TODT H.

Abstract (from CDS):

Context. The first directly detected gravitational waves (GW 150914) were emitted by two coalescing black holes (BHs) with masses of ~=36M☉ and ~=29M☉. Several scenarios have been proposed to put this detection into an astrophysical context. The evolution of an isolated massive binary system is among commonly considered models.
Aims. Various groups have performed detailed binary-evolution calculations that lead to BH merger events. However, the question remains open as to whether binary systems with the predicted properties really exist. The aim of this paper is to help observers to close this gap by providing spectral characteristics of massive binary BH progenitors during a phase where at least one of the companions is still non-degenerate.
Methods. Stellar evolution models predict fundamental stellar parameters. Using these as input for our stellar atmosphere code (Potsdam Wolf-Rayet), we compute a set of models for selected evolutionary stages of massive merging BH progenitors at different metallicities.
Results. The synthetic spectra obtained from our atmosphere calculations reveal that progenitors of massive BH merger events start their lives as O2-3V stars that evolve to early-type blue supergiants before they undergo core-collapse during the Wolf-Rayet phase. When the primary has collapsed, the remaining system will appear as a wind-fed high-mass X-ray binary. Based on our atmosphere models, we provide feedback parameters, broad band magnitudes, and spectral templates that should help to identify such binaries in the future.
Conclusions. While the predicted parameter space for massive BH binary progenitors is partly realized in nature, none of the known massive binaries match our synthetic spectra of massive BH binary progenitors exactly. Comparisons of empirically determined mass-loss rates with those assumed by evolution calculations reveal significant differences. The consideration of the empirical mass-loss rates in evolution calculations will possibly entail a shift of the maximum in the predicted binary-BH merger rate to higher metallicities, that is, more candidates should be expected in our cosmic neighborhood than previously assumed.

Abstract Copyright: © ESO, 2018

Journal keyword(s): gravitational waves - binaries: close - stars: early-type - stars: atmospheres - stars: winds, outflows - stars: mass-loss

Simbad objects: 36

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Number of rows : 36
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 MCG-03-01-015 G 00 01 57.9 -15 27 50   11.50 11.10 10.93   ~ 782 2
2 [BWF97] IC 10 X-1 HXB 00 20 29.03310480 +59 16 51.7609560           ~ 180 0
3 SMC AB 1 WR* 00 43 42.3082596960 -73 28 55.259220360 14.33 15.20 15.24   15.21 WN3+O4: 37 0
4 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
5 SMC AB 9 WR* 00 54 32.1559137576 -72 44 35.666609568 14.31 15.26 15.43   15.69 WN3ha 36 0
6 CXOU J005510.0-374212 HXB 00 55 09.990 -37 42 12.16     22.44     WNE 139 1
7 Cl* NGC 346 ELS 7 * 00 58 57.3961905528 -72 10 33.660822720 12.68 13.82 14.13   14.28 O4V((f+)) 61 0
8 Cl* NGC 346 W 3 * 00 59 00.7591806336 -72 10 28.171806492 11.46 12.61 12.80   13.63 O2III(f) 69 0
9 Cl* NGC 346 NMC 28 * 00 59 01.8187292184 -72 10 31.216864152   13.95 14.18     O5.5V((f+)) 38 0
10 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 419 1
11 SMC AB 12 WR* 01 02 52.4011237800 -72 06 52.532688348   16 16.08     WN3ha 25 0
12 IC 1613 GiC 01 04 48.4071 +02 07 10.185   10.42 10.01 9.77   ~ 1316 2
13 [AM85] IC 1613 6 WR* 01 05 01.6177966440 +02 04 19.938198792     20.7     WO3 22 1
14 [BUG2007] A 13 * 01 05 06.2582828976 +02 10 43.265668440     19.02   19.26 O3/4V((f)) 14 0
15 SK 183 * 01 29 24.5481468144 -73 33 16.345873296   13.57 13.80     O3V((f*))z+OB 23 0
16 LIN 547 WR* 01 31 04.1367366432 -73 25 03.784411524   12.75 12.90     WO4+O4V 104 0
17 NAME Phoenix Dwarf Galaxy Sy1 01 51 06.3 -44 26 41   13.48 13.2 12.69   ~ 575 2
18 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
19 [MLD95] LMC 1-550 * 05 31 11.854 -71 04 10.10 12.207 12.941 13.231   13.285 O5V 6 0
20 2MASS J05391091-6906135 * 05 39 10.9163642088 -69 06 13.739103756 14.314 15.101 15.011   14.676 O3Vn((f*)) 14 0
21 HD 46223 Y*O 06 32 09.3068103600 +04 49 24.705695568 6.73 7.50 7.28 6.95 6.79 O4V((f)) 406 0
22 Mrk 116 AGN 09 34 02.1 +55 14 25           ~ 1179 1
23 Z 36-12 H2G 10 00 00.8217342072 +05 20 09.533389560 12.77 12.25 11.89 11.71   ~ 569 0
24 Z 64-73 G 10 08 28.12 +12 18 23.4   11.3 10.0     ~ 1284 1
25 MCG-01-26-030 H2G 10 11 00.5 -04 41 30 12.48 12.13 11.93 11.78   ~ 789 2
26 HD 93128 SB* 10 43 54.3957741024 -59 32 57.497266716 8.82 8.97 8.77 9.40 8.71 O3.5V((fc))z 112 1
27 HD 93250 ** 10 44 45.0275085072 -59 33 54.680974848 6.73 8.12 7.50 8.38   O4III(fc) 334 0
28 HD 303308 ** 10 45 05.9147911152 -59 40 05.925360036 7.45 8.30 8.17 7.92 7.75 O4.5V((fc)) 314 0
29 CXOU J123030.4+413852 HXB 12 30 30.3 +41 38 53           ~ 12 0
30 [JRW2005b] 122 UX? 14 03 32.38 +54 21 03.0   21.13       ~ 120 0
31 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2
32 SN 2009ip s*b 22 23 08.26 -28 56 52.4           LBV 406 0
33 GrW 151226 GWE ~ ~           ~ 275 1
34 GrW 170104 GWE ~ ~           ~ 186 1
35 GrW 150914 GWE ~ ~           ~ 674 1
36 NAME Local Group GrG ~ ~           ~ 9325 0

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