2010ApJ...722..311L


Query : 2010ApJ...722..311L

2010ApJ...722..311L - Astrophys. J., 722, 311-328 (2010/October-2)

Discovery of a highly unequal-mass binary T dwarf with Keck laser guide star adaptive optics: a coevality test of substellar theoretical models and effective temperatures.

LIU M.C., DUPUY T.J. and LEGGETT S.K.

Abstract (from CDS):

Highly unequal-mass ratio binaries are rare among field brown dwarfs, with the mass ratio distribution of the known census described by q (4.9±0.7). However, such systems enable a unique test of the joint accuracy of evolutionary and atmospheric models, under the constraint of coevality for the individual components (the "isochrone test"). We carry out this test using two of the most extreme field substellar binaries currently known, the T1 + T6 ε Ind Bab binary and a newly discovered 0{farcs}14 T2.0 + T7.5 binary, 2MASS J12095613-1004008AB, identified with Keck laser guide star adaptive optics. The latter is the most extreme tight binary resolved to date (q ≈ 0.5). Based on the locations of the binary components on the Hertzsprung-Russell (H-R) diagram, current models successfully indicate that these two systems are coeval, with internal age differences of log(age) = -0.8±1.3(-1.0+1.2 –1.3) dex and 0.5+0.4–0.3(0.3+0.3–0.4) dex for 2MASS J1209-1004AB and ε Ind Bab, respectively, as inferred from the Lyon (Tucson) models. However, the total mass of ε Ind Bab derived from the H-R diagram (≈ 80 MJup using the Lyon models) is strongly discrepant with the reported dynamical mass. This problem, which is independent of the assumed age of the ε Ind Bab system, can be explained by a ≈ 50-100 K systematic error in the model atmosphere fitting, indicating slightly warmer temperatures for both components; bringing the mass determinations from the H-R diagram and the visual orbit into consistency leads to an inferred age of ≈ 6 Gyr for ε Ind Bab, older than previously assumed. Overall, the two T dwarf binaries studied here, along with recent results from T dwarfs in age and mass benchmark systems, yield evidence for small (≈ 100 K) errors in the evolutionary models and/or model atmospheres, but not significantly larger. Future parallax, resolved spectroscopy, and dynamical mass measurements for 2MASS J1209-1004AB will enable a more stringent application of the isochrone test. Finally, the binary nature of this object reduces its utility as the primary T3 near-IR spectral typing standard; we suggest SDSS J1206+2813 as a replacement.

Abstract Copyright: ∼

Journal keyword(s): binaries: close - binaries: general - brown dwarfs - infrared: stars - techniques: high angular resolution

Simbad objects: 40

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Number of rows : 40
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 NAME L 362-29 BC BD* 00 04 34.8671722377 -40 44 06.463544237       19.61 16.88 L5+L5 119 0
2 2MASSI J0025036+475919 BD* 00 25 03.65928 +47 59 19.1868           L4: 25 0
3 LP 349-25 SB* 00 27 56.0057038615 +22 19 32.635434516   18.6   16.0   M8Ve 82 0
4 DENIS J004135.3-562112 LM* 00 41 35.3862348768 -56 21 12.872262132       17.97 14.69 M7.5e 39 0
5 DENIS J020529.0-115925 BD* 02 05 29.3651195393 -11 59 29.721210536           L7V 156 0
6 2MASSW J0310599+164816 BD* 03 10 59.86560 +16 48 15.5988           L8V 57 0
7 2MASS J03572695-4417305 BD* 03 57 26.9613211008 -44 17 30.532793208         17.86 L0beta 43 1
8 2MASSI J0423485-041403 BD* 04 23 48.5763811987 -04 14 03.246502948           L6.5+T2 137 0
9 2MASS J05185995-2828372 BD* 05 18 59.95656 -28 28 37.2720           L6+T4 41 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 * pi.01 Cnc C BD* 09 12 14.69112 +14 59 39.6240           L8.5+L7.5 61 1
12 2MASS J09153413+0422045 BD* 09 15 34.13712 +04 22 04.5948           L6 42 0
13 2MASSW J0920122+351742 BD* 09 20 12.23664 +35 17 42.9684           L5.5+L9 52 0
14 2MASS J09261537+5847212 BD* 09 26 15.37752 +58 47 21.2280           T3.5+T5 39 0
15 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 79 0
16 2MASS J10521350+4422559 BD* 10 52 13.50504 +44 22 55.9128           L6.5+T1.5 38 0
17 HD 97334B BD* 11 12 25.6353966120 +35 48 12.742807176           L4.5+L6 95 0
18 2MASS J11463449+2230527 BD* 11 46 34.5341033040 +22 30 54.036482400           L3+L4 94 0
19 2MASS J12095613-1004008 BD* 12 09 56.13096 -10 04 00.8076           T2+T7.5 67 0
20 2MASS J12255432-2739466 BD* 12 25 54.32328 -27 39 46.6776           T5.5+T8 67 0
21 SIPS J1228-1547 BD* 12 28 15.23184 -15 47 34.2312       20.414 18.042 L5.5+L5.5 151 0
22 2MASSW J1239272+551537 BD* 12 39 27.27287 +55 15 37.1630           L5V 47 0
23 NAME Kelu-1 BD* 13 05 40.1642434199 -25 41 05.712165150         16.85 L2+L3.5 267 0
24 2MASS J14044948-3159330 BD* 14 04 49.48416 -31 59 33.0576           T1+T5 35 1
25 2MASS J14162408+1348263 BD* 14 16 24.0739698960 +13 48 26.193281184           L5 88 1
26 NAME HD 130948BC BD* 14 50 16.00 +23 54 41.8           L4+L4 75 0
27 BD+16 2708B SB* 14 54 29.4185719182 +16 06 08.616294953           M8.5 143 0
28 2MASS J15341711+1615463 BD* 15 34 17.11008 +16 15 46.3680           T1.5+T5.5 25 0
29 2MASSI J1534498-295227 BD* 15 34 49.84080 -29 52 27.4188           T4.5+T5 73 0
30 2MASS J15530228+1532369 BD* 15 53 02.28072 +15 32 36.9132           T6.5+T7.5 63 0
31 2MASSW J1728114+394859 BD* 17 28 11.50056 +39 48 59.3100           L5+L6.5 65 0
32 SDSS J205235.31-160929.8 BD* 20 52 35.31672 -16 09 29.8620           L8.5+T1.5 23 0
33 2MASSW J2101154+175658 BD* 21 01 15.44112 +17 56 58.6860           L7+L8 34 0
34 2MASS J21321145+1341584 BD* 21 32 11.45376 +13 41 58.4124           L4.5+L8.5 29 0
35 2MASS J21522609+0937575 BD* 21 52 26.09064 +09 37 57.5328           L6+L6 25 0
36 * eps Ind PM* 22 03 21.6536261624 -56 47 09.522795714   5.75 4.69     K5V 616 0
37 * eps Ind B BD* 22 04 10.5951812451 -56 46 58.239102418     24.12 20.8 15.60 T1V+T6V 176 1
38 2MASS J22495345+0044046 BD* 22 49 53.45592 +00 44 04.6608           L3+L5 49 0
39 2MASS J22521073-1730134 BD* 22 52 10.7512306563 -17 30 13.889743018         17.9 L4.5+T3.5 64 1
40 SIPS J2255-5713 BD* 22 55 18.5785255822 -57 13 06.200631761       20.58   L6:+L8 24 0

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