2010ApJ...711.1087K


Query : 2010ApJ...711.1087K

2010ApJ...711.1087K - Astrophys. J., 711, 1087-1122 (2010/March-2)

High-precision dynamical masses of very low mass binaries.

KONOPACKY Q.M., GHEZ A.M., BARMAN T.S., RICE E.L., BAILEY III J.I., WHITE R.J., McLEAN I.S. and DUCHENE G.

Abstract (from CDS):

We present the results of a three year monitoring program of a sample of very low mass (VLM) field binaries using both astrometric and spectroscopic data obtained in conjunction with the laser guide star adaptive optics system on the W. M. Keck II 10 m telescope. Among the 24 systems studied, 15 have undergone sufficient orbital motion, allowing us to derive their relative orbital parameters and hence their total system mass. These measurements more than double the number of mass measurements for VLM objects, and include the most precise mass measurement to date (<2%). Among the 11 systems with both astrometric and spectroscopic measurements, six have sufficient radial velocity variations to allow us to obtain individual component masses. This is the first derivation of the component masses for five of these systems. Altogether, the orbital solutions of these low mass systems show a correlation between eccentricity and orbital period, consistent with their higher mass counterparts. In our primary analysis, we find that there are systematic discrepancies between our dynamical mass measurements and the predictions of theoretical evolutionary models (TUCSON and LYON) with both models either underpredicting or overpredicting the most precisely determined dynamical masses. These discrepancies are a function of spectral type, with late-M through mid-L systems tending to have their masses underpredicted, while one T-type system has its mass overpredicted. These discrepancies imply that either the temperatures predicted by evolutionary and atmosphere models are inconsistent for an object of a given mass, or the mass-radius relationship or cooling timescales predicted by the evolutionary models are incorrect. If these spectral-type trends are correct and hold into the planetary mass regime, the implication is that the masses of directly imaged extrasolar planets are overpredicted by the evolutionary models.

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Journal keyword(s): binaries: visual - brown dwarfs - stars: fundamental parameters - stars: low-mass - techniques: high angular resolution

Simbad objects: 38

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Number of rows : 38
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 LP 349-25 SB* 00 27 56.0057038615 +22 19 32.635434516   18.6   16.0   M8Ve 82 0
2 * 74 Psc B PM* 01 05 41.7111106896 +21 27 55.612006704   5.405 5.455     B9IVn 76 0
3 LP 415-20 LM* 04 21 49.5764748384 +19 29 08.566062612           M7+M9.5 56 0
4 * 18 Ori * 05 16 04.1346616440 +11 20 28.878184140   5.500 5.515     A0V 73 0
5 2MASS J05185995-2828372 BD* 05 18 59.95656 -28 28 37.2720           L6+T4 41 0
6 2MASS J06523073+4710348 BD* 06 52 30.7182715296 +47 10 34.926594456           L5.0 50 0
7 2MASS J07003664+3157266 BD* 07 00 36.7233300485 +31 57 25.462866965           L3+L6.5 52 0
8 LSPM J0746+2000 BD* 07 46 42.56207 +20 00 32.1839       17.9 15.034 L0+L1.5 201 1
9 HD 71906 * 08 31 19.9662429960 +37 15 53.796537612   6.127 6.174     A0V 62 0
10 2MASS J08503593+1057156 BD* 08 50 35.93400 +10 57 15.6168       22.466 20.349 L6.5+L8.5 85 0
11 2MASSW J0920122+351742 BD* 09 20 12.23664 +35 17 42.9684           L5.5+L9 52 0
12 2MASS J10170754+1308398 BD* 10 17 07.5535371936 +13 08 39.784300548         17.418 L1.5+L3 34 0
13 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 79 0
14 LP 213-67 LM* 10 47 12.6095390983 +40 26 43.737443862   19.2       M6.5Ve 47 1
15 HD 97334B BD* 11 12 25.6353966120 +35 48 12.742807176           L4.5+L6 95 0
16 LP 732-94 SB* 11 21 49.1708652037 -13 13 08.693807585     19.57     M8.5V 147 1
17 * eta Crt PM* 11 56 00.9541135272 -17 09 02.968088832   5.138 5.160     A0V 75 0
18 * q Vir PM* 12 33 46.7485436339 -09 27 07.478534302   5.45 5.48     B9V 79 0
19 2MASSI J1426316+155701 LM* 14 26 31.6133387736 +15 57 01.066079268       18.320 15.819 M9V 32 0
20 NAME HD 130948BC BD* 14 50 16.00 +23 54 41.8           L4+L4 75 0
21 BD+16 2708 PM* 14 54 29.2361840107 +16 06 03.797990080 12.86 11.686 10.150 9.116 7.872 M3V 305 1
22 BD+16 2708B SB* 14 54 29.4185719182 +16 06 08.616294953           M8.5 143 0
23 HD 131951 * 14 56 13.2300928608 +14 26 46.540838544   5.862 5.892     A0V 66 0
24 2MASSI J1534498-295227 BD* 15 34 49.84080 -29 52 27.4188           T4.5+T5 73 0
25 2MASSI J1600054+170832 BD* 16 00 05.4775186992 +17 08 32.725071672           L1.5V 15 0
26 2MASSW J1728114+394859 BD* 17 28 11.50056 +39 48 59.3100           L5+L6.5 65 0
27 HD 162132 SB* 17 47 08.0338354344 +47 36 44.093422656   6.549 6.465   6.37 A2Vs 77 0
28 LSPM J1750+4424 LM* 17 50 12.9048979032 +44 24 04.388509332   21.0   18.8   M6.5+M8.5 26 0
29 2MASSI J1847034+552243 SB* 18 47 03.4341091776 +55 22 43.458679704   18.7   16.4   M6+M7 15 0
30 * 51 Dra * 19 04 55.1654401944 +53 23 47.960875608   5.37 5.38     A0Vn 60 0
31 2MASSW J2101154+175658 BD* 21 01 15.44112 +17 56 58.6860           L7+L8 34 0
32 2MASS J21402931+1625183 ** 21 40 29.3219106816 +16 25 18.097174704         15.36 M8+M9.5 35 0
33 2MASS J21522609+0937575 BD* 21 52 26.09064 +09 37 57.5328           L6+L6 25 0
34 HD 208108 * 21 53 37.3886477424 +19 40 06.479949432   5.693 5.676     A0Vs 69 0
35 2MASSW J2206228-204705 SB* 22 06 22.8297746064 -20 47 06.597790152     19.788 17.452 14.877 M8.0V 50 0
36 HD 210780 Ro* 22 13 09.4258527480 -21 24 21.588767136   8.39 8.34     B9.5/A0V 19 0
37 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0
38 HD 222332 * 23 39 41.5645602720 -22 32 00.169439136   7.41 7.29     A0V 19 0

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