2017ApJS..230...15M


Query : 2017ApJS..230...15M

2017ApJS..230...15M - Astrophys. J., Suppl. Ser., 230, 15-15 (2017/June-0)

Mind your Ps and Qs: the interrelation between period (P) and mass-ratio (q) distributions of binary stars.

MOE M. and DI STEFANO R.

Abstract (from CDS):

We compile observations of early-type binaries identified via spectroscopy, eclipses, long-baseline interferometry, adaptive optics, common proper motion, etc. Each observational technique is sensitive to companions across a narrow parameter space of orbital periods P and mass ratios q = Mcomp/M1. After combining the samples from the various surveys and correcting for their respective selection effects, we find that the properties of companions to O-type and B-type main-sequence (MS) stars differ among three regimes. First, at short orbital periods P <= 20 days (separations a <= 0.4 au), the binaries have small eccentricities e <= 0.4, favor modest mass ratios <q>~0.5, and exhibit a small excess of twins q > 0.95. Second, the companion frequency peaks at intermediate periods log P (days) ≃ 3.5 (a ≃ 10 au), where the binaries have mass ratios weighted toward small values q ≃ 0.2-0.3 and follow a Maxwellian "thermal" eccentricity distribution. Finally, companions with long orbital periods log P (days) ≃ 5.5-7.5 (a ≃ 200-5000 au) are outer tertiary components in hierarchical triples and have a mass ratio distribution across q ≃ 0.1-1.0 that is nearly consistent with random pairings drawn from the initial mass function. We discuss these companion distributions and properties in the context of binary-star formation and evolution. We also reanalyze the binary statistics of solar-type MS primaries, taking into account that 30% ± 10% of single-lined spectroscopic binaries likely contain white dwarf companions instead of low-mass stellar secondaries. The mean frequency of stellar companions with q > 0.1 and log P (days) < 8.0 per primary increases from 0.50 ± 0.04 for solar-type MS primaries to 2.1 ± 0.3 for O-type MS primaries. We fit joint probability density functions f(M1,q,P,e)≠f(M1)f(q)f(P)f(e) to the corrected distributions, which can be incorporated into binary population synthesis studies.

Abstract Copyright: © 2017. The American Astronomical Society. All rights reserved.

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

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 * zet Phe SB* 01 08 23.0805843521 -55 14 44.736015873   3.908 4.014     B6V+B9V 243 0
2 HD 13445 PM* 02 10 25.9181700303 -50 49 25.465181208   6.945 6.117     K1.5V 484 1
3 HD 15136 * 02 28 23.8001711136 +56 15 13.458649104   9.11 8.85     A1III 8 0
4 * gam Cet ** 02 43 18.03910 +03 14 08.9390 3.63 3.56 3.47 3.36 3.32 A2Vn+F4V 185 0
5 * pi. Ari ** 02 49 17.55924 +17 27 51.5168 4.68         B6V 104 0
6 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
7 HD 18537 Pu* 03 00 52.2110264304 +52 21 06.248122308 4.78 5.158 5.219     B7V 87 0
8 Cl Melotte 20 MGr 03 26 50.6 +48 51 48           ~ 928 0
9 * tau05 Eri SB* 03 33 47.2758917450 -21 37 58.384116886   4.15 4.25     B9V 115 0
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
11 NGC 2168 OpC 06 09 07.5 +24 20 15           ~ 604 0
12 HD 54662 SB* 07 09 20.2493151288 -10 20 47.635088964 5.35 6.24 6.21 7.23   O6.5Vz(n)+O7.5Vz 354 0
13 NGC 2632 OpC 08 39 58.4 +19 36 33           ~ 1733 0
14 HD 93161A SB* 10 44 08.8380609288 -59 34 34.509718560 7.33 8.619 8.581 8.61   O7.5V+O9V 52 1
15 HD 93161 ** 10 44 08.97168 -59 34 34.8780 7.39 7.96 7.87     O8V+O9V+O6.5(f) 97 0
16 HD 93161B * 10 44 09.0755469120 -59 34 35.393294136   8.658 8.641     O6.5IV((f)) 24 1
17 HD 93222 Y*O 10 44 36.2481200208 -60 05 28.890759120 7.26 8.18 8.10 8.91   O7V((f))z 212 0
18 * eps Cen bC* 13 39 53.25774 -53 27 59.0081 1.16 2.08 2.30 2.45 2.70 B1III 259 0
19 HD 123590 * 14 10 43.9689754248 -62 28 44.450066712 6.93 9.21 8.84 8.68   O8Vz 45 0
20 * alf CrB SB* 15 34 41.2684881676 +26 42 52.866000089 2.19 2.22 2.24 2.21 2.25 A1IV 499 0
21 HD 144987 PM* 16 09 52.5898714152 -33 32 44.903550228   5.410 5.497     B8V 45 0
22 NAME Upper Sco-Cen As* 16 15 -24.2           ~ 1497 1
23 HD 150136 SB* 16 41 20.4155898816 -48 45 46.730465028 4.98 5.78 5.65 6.93   O3.5-4III(f*)+O6IV 201 0
24 HD 152246 SB* 16 54 05.2976157264 -41 04 46.117795944 6.69 7.45 7.29 8.19   O9IV 132 1
25 HD 152314 ** 16 54 32.0048577720 -41 48 18.848961036 7.256 7.974 7.749 9.01 7.446 O9IV 113 0
26 * e Her PM* 17 17 40.2531980520 +37 17 29.422635288 4.67 4.70 4.65 4.56 4.56 A2V 100 0
27 * kap Sco bC* 17 42 29.27520 -39 01 47.9391 1.32 2.211 2.386     B1.5III 250 0
28 * 9 Sgr Y*O 18 03 52.4450051016 -24 21 38.632254012 5.08 5.97 5.97 5.72 5.70 O4V((f))z 563 0
29 M 16 OpC 18 18 45.1 -13 47 31           ~ 1084 1
30 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
31 * 71 Dra SB* 20 19 36.7272071568 +62 15 26.797556412   5.660 5.709     B9V 83 0
32 Ass Cyg OB 2 As* 20 33.2 +41 19           ~ 1023 0
33 HD 239649 * 21 23 34.5595066128 +59 51 05.432338980   9.47 9.34     B8 19 0
34 Ass Cep OB 2 As* 21 51 +60.0           ~ 303 0
35 BD+61 2218 Y*? 21 54 01.6859879520 +62 37 09.498981936   10.10 10.04     B5V 19 0
36 * psi03 Aqr * 23 18 57.6766613352 -09 36 38.695365432   4.977 5.003     B9V 87 0

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