2010ApJ...719.1293K


Query : 2010ApJ...719.1293K

2010ApJ...719.1293K - Astrophys. J., 719, 1293-1314 (2010/August-3)

High-precision orbital and physical parameters of double-lined spectroscopic binary stars - HD78418, HD123999, HD160922, HD200077, and HD210027.

KONACKI M., MUTERSPAUGH M.W., KULKARNI S.R. and HELMINIAK K.G.

Abstract (from CDS):

We present high-precision radial velocities (RVs) of double-lined spectroscopic binary stars HD78418, HD123999, HD160922, HD200077, and HD210027. They were obtained based on the high-resolution echelle spectra collected with the Keck I/HIRES, Shane/CAT/Hamspec, and TNG/Sarge telescopes/spectrographs over the years 2003-2008 as part of the TATOOINE search for circumbinary planets. The RVs were computed using our novel iodine cell technique for double-line binary stars, which relies on tomographically disentangled spectra of the components of the binaries. The precision of the RVs is of the order of 1-10 m/s, and to properly model such measurements one needs to account for the light-time effect within the binary's orbit, relativistic effects, and RV variations due to tidal distortions of the components of the binaries. With such proper modeling, our RVs combined with the archival visibility measurements from the Palomar Testbed Interferometer (PTI) allow us to derive very precise spectroscopic/astrometric orbital and physical parameters of the binaries. In particular, we derive the masses, the absolute K- and H-band magnitudes, and the parallaxes. The masses together with the absolute magnitudes in the K and H bands enable us to estimate the ages of the binaries. These RVs allow us to obtain some of the most accurate mass determinations of binary stars. The fractional accuracy in msin i only, and hence based on the RVs alone, ranges from 0.02% to 0.42%. When combined with the PTI astrometry, the fractional accuracy in the masses in the three best cases ranges from 0.06% to 0.5%. Among them, the masses of HD210027 components rival in precision the mass determination of the components of the relativistic double pulsar system PSR J0737-3039. In the near future, for double-lined eclipsing binary stars we expect to derive masses with a fractional accuracy of the order of up to ∼0.001% with our technique. This level of precision is an order of magnitude higher than of the most accurate mass determination for a body outside the solar system–the double neutron star system PSR B1913+16.

Abstract Copyright: ∼

Journal keyword(s): binaries: spectroscopic - stars: fundamental parameters - stars: individual (HD78418, HD123999, HD160922, HD200077, HD210027) - techniques: radial velocities

VizieR on-line data: <Available at CDS (J/ApJ/719/1293): table1.dat table4.dat>

Simbad objects: 32

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Number of rows : 32
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 * 64 Psc SB* 00 48 58.7075574408 +16 56 26.324381004   5.58   4.8   F8V 149 0
2 V* AI Phe SB* 01 09 34.1924055096 -46 15 56.071719360   9.26 8.60     F7V+K0IV 157 0
3 * bet Per SB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1265 1
4 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
5 * 1 LMi * 08 38 18.9811480848 +32 48 07.260579288   7.062 5.950     K2III: 29 0
6 * 75 Cnc SB* 09 08 47.3310550733 +26 37 44.817238087   6.62 5.95 5.5   G5IV-V 145 0
7 * 19 UMa HB* 09 15 14.2459147392 +34 38 00.659017644       5.5   G6III 157 0
8 * omi Leo SB* 09 41 09.0321741326 +09 53 32.308426423 4.22 4.01 3.52 3.11 2.88 F8-G0III+A7m 163 0
9 * zet UMa ** 13 23 55.54048 +54 55 31.2671           ~ 93 0
10 * 7 Boo * 13 53 12.9300854664 +17 55 58.327270932   6.551 5.709     G5III 74 0
11 HD 123612 * 14 08 15.8599574352 +24 18 54.180012276   8.040 6.544     K5III 25 0
12 * d Boo SB* 14 10 23.9334932664 +25 05 30.037020972 5.44 5.37 4.83 4.39 4.10 F8V 180 0
13 * sig Boo PM* 14 34 40.8173867232 +29 44 42.457673940 4.76 4.84 4.47 4.13 3.94 F4VkF2mF1 632 0
14 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
15 HD 154633 * 17 02 15.7477043808 +64 36 02.667219876   7.070 6.094     G5V 53 0
16 HD 158633 PM* 17 25 00.0977414147 +67 18 24.148745592   7.19   5.9   K0 224 0
17 * ome Dra SB* 17 36 57.0943076755 +68 45 28.681533966   5.20 4.77 4.5   F4V 180 0
18 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
19 * 36 Dra PM* 18 13 53.8328065738 +64 23 50.225760192   5.407 4.987 4.8   F5V 215 0
20 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
21 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
22 * sig Dra PM* 19 32 21.5902098601 +69 39 40.235805206 5.860 5.460 4.680 4.04 3.63 K0V 691 0
23 * b03 Cyg dS* 20 14 32.0323540824 +36 48 22.700909124 5.10 5.11 4.99 4.79 4.72 A2V 284 0
24 HD 192985 PM* 20 16 00.6155322192 +45 34 46.290085536   6.281 5.864     F5V: 94 0
25 HD 199763 PM* 20 58 15.5718528216 +30 23 45.372340608   7.57 6.54     G9III 14 0
26 HD 200077 SB* 20 59 55.2757447771 +40 15 31.757352772   7.136 6.593 7.32   F8 79 0
27 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2
28 * iot Peg SB* 22 07 00.6655101792 +25 20 42.356386464 4.190 4.200 3.770 3.36 3.11 F5V 468 1
29 * pi. Peg RG* 22 09 59.2430193207 +33 10 41.600399246 4.93 4.75 4.29 3.90 3.63 F5II-III_sh 140 0
30 HD 211006 PM* 22 13 38.6985335160 +28 36 28.859310360   7.037 5.867     K2III 48 0
31 HD 211432 * 22 16 29.6467539432 +27 48 14.506673004   7.372 6.370     G9III 23 0
32 * 45 Peg PM* 22 45 28.1758730160 +19 21 59.604955380   7.326 6.269     G6III: 41 0

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