2023A&A...672A..22B


Query : 2023A&A...672A..22B

2023A&A...672A..22B - Astronomy and Astrophysics, volume 672A22 (2023/4-1)

The IACOB project VIII. Searching for empirical signatures of binarity in fast-rotating O-type stars.

BRITAVSKIY N., SIMON-DIAZ S., HOLGADO G., BURSSENS S., MAIZ APELLANIZ J., ELDRIDGE J.J., NAZE Y., PANTALEONI GONZALEZ M. and HERRERO A.

Abstract (from CDS):

Context. The empirical distribution of projected rotational velocities (v sin i) in massive O-type stars is characterised by a dominant slow velocity component and a tail of fast rotators. It has been proposed that binary interaction plays a dominant role in the formation of this tail.
Aims. We perform a complete and homogeneous search for empirical signatures of binarity in a sample of 54 fast-rotating stars with the aim of evaluating this hypothesis. This working sample has been extracted from a larger sample of 415 Galactic O-type stars that covers the full range of v sin i values.
Methods. We used new and archival multi-epoch spectra in order to detect spectroscopic binary systems. We complemented this information with Gaia proper motions and TESS photometric data to aid in the identification of runaway stars and eclipsing binaries, respectively. We also benefitted from additional published information to provide a more complete overview of the empirical properties of our working sample of fast-rotating O-type stars.
Results. The identified fraction of single-lined spectroscopic binary (SB1) systems and apparently single stars among the fast-rotating sample is ∼18% and ∼70%, respectively. The remaining 12% correspond to four secure double-line spectroscopic binaries (SB2) with at least one of the components having a v sin i > 200 km s–1 (∼8%), along with a small sample of 2 stars (∼4%) for which the SB2 classification is doubtful: these could actually be single stars with a remarkable line-profile variability. When comparing these percentages with those corresponding to the slow-rotating sample, we find that our sample of fast rotators is characterised by a slightly larger percentage of SB1 systems (∼18% vs. ∼13%) and a considerably smaller fraction of clearly detected SB2 systems (8% vs. 33%). Overall, there seems to be a clear deficit of spectroscopic binaries (SB1+SB2) among fast-rotating O-type stars (∼26% vs. ∼46%). On the contrary, the fraction of runaway stars is significantly higher in the fast-rotating domain (∼33-50%) than among those stars with v sin i < 200 km s–1. Lastly, almost 65% of the apparently single fast-rotating stars are runaways. As a by-product, we discovered a new over-contact SB2 system (HD 165921) and two fast-rotating SB1 systems (HD 46485 and HD 152200) Also, we propose HD 94024 and HD 12323 (both SB1 systems with a v sin i < 200 km s–1) as candidates for hosting a quiescent stellar-mass black hole.
Conclusions. Our empirical results seem to be in good agreement with the assumption that the tail of fast-rotating O-type stars (with v sin i > 200 km s–1) is mostly populated by post-interaction binary products. In particular, we find that the final statistics of identified spectroscopic binaries and apparent single stars are in good agreement with newly computed predictions obtained with the binary population synthesis code BPASS and earlier estimations obtained in previous studies.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: early-type - stars: rotation - stars: oscillations - stars: fundamental parameters - techniques: spectroscopic - binaries: spectroscopic

VizieR on-line data: <Available at CDS (J/A+A/672/A22): tablea.dat tableb.dat>

Simbad objects: 68

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Number of rows : 68
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 BD+60 134 * 00 56 14.2146529032 +61 45 36.974823444 11 11.29 10.6     O5.5V(n)((f)) 30 0
2 HD 5689 * 00 59 47.5908405456 +63 36 28.250542152 8.79 9.41 9.19     O7Vn((f)) 60 0
3 HD 12323 SB* 02 02 30.1268458032 +55 37 26.372271540 7.95 8.87 8.92     ON9.2V 193 0
4 HD 13268 * 02 11 29.7003301008 +56 09 31.721738760 7.48 8.24 8.18     ON8.5IIIn 186 0
5 Ass Per OB 1 As* 02 21 +57.6           ~ 181 1
6 HD 14434 Em* 02 21 52.4121560832 +56 54 18.032028876 7.87 8.65 8.49 8.29 8.20 O5.5Vnn((f))p 198 0
7 HD 14442 V* 02 22 10.7004415512 +59 32 58.893287604 9.01 9.58 9.27     O5n(f)p 110 0
8 HD 15137 SB* 02 27 59.8113542520 +52 32 57.589857672 7 7.92 7.86     O9.5II-IIIn 143 0
9 BD+60 498 Y*O 02 32 10.8542551368 +61 33 07.940208384 11.61 10.47 9.94     O9V 113 0
10 HD 15642 * 02 32 56.3830465728 +55 19 39.055987236 9.305 8.56 8.55     O9.5II-IIIn 110 0
11 BD+60 513 Y*O 02 34 02.5297182912 +61 23 10.877763048 9.38 9.88 9.39     O7Vnz 116 0
12 * ksi Per ** 03 58 57.9024302099 +35 47 27.709515737 3.190 4.080 4.060 3.88 3.89 O7.5III(n)((f)) 850 0
13 * 1 Cam A * 04 32 01.8407070864 +53 54 39.015769176   5.87 5.77 6.71   O9.7IIn 14 0
14 * del Ori ** 05 32 00.40009 -00 17 56.7424 0.96 2.02 2.41 2.32 2.54 O9.5IINwk 796 0
15 HD 36879 * 05 35 40.5264730272 +21 24 11.719601856 6.97 7.69 7.58     O7V(n)((f))z 157 0
16 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
17 HD 37737 SB* 05 42 31.1584798320 +36 12 00.508318740 8.02 8.30 8.06     O9.5II-III(n) 100 0
18 HD 41161 * 06 05 52.4562749544 +48 14 57.417890532 5.66 6.658 6.764     O8Vn 139 0
19 HD 41997 * 06 08 55.8226126488 +15 42 18.192106044 8.16 9.47 9.13 8.83   O7.5Vn((f)) 108 0
20 HD 46056 Y*O 06 31 20.8608343776 +04 50 03.842554740 7.60 8.36 8.16 8.16 8.09 O8Vn 242 0
21 HD 46202 bC* 06 32 10.4706981304 +04 57 59.764912343 7.60 8.332 8.269 7.98 7.86 O9.2V 300 0
22 HD 46485 Y*O 06 33 50.9566745256 +04 31 31.613196504 7.92 8.60 8.27   8.10 O7V((f))nzvar? 162 0
23 HD 47129 SB* 06 37 24.0420854544 +06 08 07.369104444 5.23 6.11 6.06     O8I+O7.5III 420 0
24 * 15 Mon Be* 06 40 58.65963 +09 53 44.7229 3.360 4.45 4.68   4.88 O7V+B1.5/2V 823 0
25 HD 52266 SB* 07 00 21.0763468632 -05 49 35.954203044 6.32 7.22 7.23     O9.5IIIn 125 0
26 HD 52533 SB* 07 01 27.0486333888 -03 07 03.286283952 6.66 7.57 7.68     O8.5IVn 123 0
27 HD 53975 SB* 07 06 35.9651934840 -12 23 38.220633600 5.38 6.40 6.50 6.51   O7.5Vz 206 0
28 HD 76556 * 08 55 07.1436167808 -47 36 27.161751528 8.03 8.61 8.20 8.90   O6IV(n)((f))p 80 1
29 HD 89137 * 10 15 40.0854126480 -51 15 24.093239544 7.02 7.93 7.97 8.82   ON9.7II(n) 105 0
30 HD 90087 * 10 22 20.8753379544 -59 45 19.692781128 6.91 9.49 8.92 8.96   O9.2III(n) 102 1
31 HD 91651 bC* 10 33 30.2993151816 -60 07 40.044178344 7.96 9.64 9.52 9.51   ON9.5IIIn 109 0
32 HD 93521 * 10 48 23.5113981120 +37 34 13.083332412 5.67 6.79 7.03     O9.5IIInn 443 1
33 HD 94024 SB* 10 50 01.5072417792 -57 52 26.267968992 8.03 9.15 9.45 9.41   O8IV 63 0
34 HD 97434 * 11 11 49.5794597256 -60 41 58.263437472 7.45 8.24 8.07 7.95 7.79 O7.5III(n)((f)) 76 0
35 V* TU Mus SB* 11 31 10.9241479224 -65 44 32.099167788 7.58 9.52 9.34 9.25   O8V(n)z+B0V(n) 185 0
36 HD 308813 SB* 11 37 58.4451890256 -63 18 59.455147284 8.46 9.68 9.73 9.74   O9.7IV(n) 85 0
37 HD 102415 * 11 46 54.4041886200 -61 27 46.987376184 8.51 9.44 9.35 9.67   ON9IIInn 44 0
38 HD 117490 * 13 32 08.5985517168 -60 48 55.484598312 8.13 8.94 8.92 9.52   ON9.5IIInn 47 0
39 HD 124314 ** 14 15 01.60615 -61 42 24.3831   8.96 6.64 6.45 6.31 O6V(n)((f)) 155 0
40 HD 124979 * 14 18 11.9392840920 -51 30 13.855274964 7.81 8.61 8.51 9.37   O7.5IV(n)((f)) 95 1
41 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
42 * 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
43 HD 149452 * 16 37 10.5115048704 -47 07 49.828653588 9.2 10.39 9.40 9.54 8.73 O9IVn 59 0
44 HD 152200 SB* 16 53 51.6564464880 -41 50 32.716447224 7.744 8.488 8.391 9.31 8.152 O9.7IV(n) 73 0
45 HD 326331 SB* 16 54 25.9691286216 -41 49 55.768191852 6.886 7.678 7.497   7.143 O8IVn((f)) 87 0
46 V* V1297 Sco SB* 16 56 05.2157203176 -40 20 57.576260184 7.87 9.11 9.29 9.29   O7.5Vz 149 0
47 HD 155913 * 17 16 26.3328574536 -42 40 04.122580080 8.2 8.81 8.34 9.05   O4.5Vn((f)) 63 0
48 HD 163892 SB* 17 59 26.3102746896 -22 28 00.861673188 6.81 7.61 7.44 8.55   O9.5IV(n) 111 0
49 V* V986 Oph bC* 18 04 37.3575698448 +01 55 08.375650428 5.23 6.082 6.147     O9.7IIn 121 0
50 HD 165246 SB* 18 06 04.6792554840 -24 11 43.890335448 6.90 7.70 7.60 8.77   O8V(n) 93 0
51 * 11 Sgr Or* 18 09 17.6999100192 -23 59 18.231196056 6.65 7.45 7.31 8.36   O7V(n)z+B0:V: 146 2
52 HD 172175 s*b 18 39 03.7744177488 -07 51 35.440779672 9.63 10.00 9.54     O6.5I(n)fp 66 0
53 V* V1182 Aql SB* 18 55 23.1255094080 +09 20 48.087475944 8.73 9.10 8.64     O7V(n)((f))z+B 119 0
54 HD 175876 * 18 58 10.7660947512 -20 25 25.541961636 5.79 6.82 6.94 6.93   O6.5III(n)(f) 154 0
55 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
56 HD 191423 * 20 08 07.1135347944 +42 36 21.962454480 7.43 8.19 8.03     ON9II-IIInn 119 0
57 V* V2011 Cyg SB* 20 12 33.1203741480 +40 16 05.445674868 7.32 7.85 7.55     O4.5V(n)((f)) 221 0
58 HD 228841 Em* 20 18 29.6946566952 +38 52 39.774824724 9.08 9.50 9.01     O6.5Vn((f)) 66 0
59 V* V382 Cyg SB* 20 18 47.2202814912 +36 20 26.085111756 9.35 9.19 8.65     O6IVn+O5Vn 201 0
60 HD 229232 SB* 20 23 59.1861751224 +39 06 15.291161496 10.17 10.303 9.500 9.330   O4Vn((f)) 44 0
61 BD+36 4145 Em* 20 36 18.2062785936 +37 25 02.815437468 9.23 9.47 8.96     O8.5V(n) 48 0
62 * 68 Cyg SB* 21 18 27.1862219256 +43 56 45.399147864 4.05 4.99 5.00     O7.5IIIn((f)) 383 0
63 * lam Cep s*b 22 11 30.5765111040 +59 24 52.154264880 4.55 5.29 5.05 4.77 4.62 O6.5I(n)fp 705 1
64 Hilt 1118 * 22 23 17.4198642168 +55 38 02.195795472 9.83 10.49 10.30     O6.5Vnn((f)) 22 0
65 HD 216532 V* 22 52 30.5558211936 +62 26 25.947105900 8.06 8.46 8.0     O8.5V(n) 149 0
66 HD 217086 Y*O 22 56 47.1887590800 +62 43 37.657173900 7.88 8.30 7.66 8.35   O7Vnn((f))z 263 0
67 BD+60 2522 Em* 23 20 44.5134945744 +61 11 40.530567984 8.46 9.08 8.67     O6.5(n)fp 228 1
68 NGC 7635 HII 23 20 48.3 +61 12 06           ~ 179 2

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