2019ApJ...882..117L


Query : 2019ApJ...882..117L

2019ApJ...882..117L - Astrophys. J., 882, 117-117 (2019/September-2)

3.8 µm imaging of 400-600 K brown dwarfs and orbital constraints for WISEP J045853.90+643452.6AB.

LEGGETT S.K., DUPUY T.J., MORLEY C.V., MARLEY M.S., BEST W.M.J., LIU M.C., APAI D., CASEWELL S.L., GEBALLE T.R., GIZIS J.E., PINEDA J.S., RIEKE M. and WRIGHT G.S.

Abstract (from CDS):

Half of the energy emitted by late-T- and Y-type brown dwarfs emerges at 3.5 <= λ µm <= 5.5. We present new L' (3.43 <= λ µm <= 4.11) photometry obtained at the Gemini North telescope for nine late-T and Y dwarfs, and synthesize L' from spectra for an additional two dwarfs. The targets include two binary systems that were imaged at a resolution of 0.''25. One of these, WISEP J045853.90+643452.6AB, shows significant motion, and we present an astrometric analysis of the binary using Hubble Space Telescope, Keck Adaptive Optics, and Gemini images. We compare λ ∼ 4 µm observations to models, and find that the model fluxes are too low for brown dwarfs cooler than ∼700 K. The discrepancy increases with decreasing temperature, and is a factor of ∼2 at Teff = 500 K and ∼4 at Teff = 400 K. Warming the upper layers of a model atmosphere generates a spectrum closer to what is observed. The thermal structure of cool brown dwarf atmospheres above the radiative-convective boundary may not be adequately modeled using pure radiative equilibrium; instead heat may be introduced by thermochemical instabilities (previously suggested for the L- to T-type transition) or by breaking gravity waves (previously suggested for the solar system giant planets). One-dimensional models may not capture these atmospheres, which likely have both horizontal and vertical pressure/temperature variations.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): astrometry - binaries: general - brown dwarfs - infrared: stars - stars: atmospheres

Simbad objects: 16

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Number of rows : 16
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 WISE J000517.48+373720.5 BD* 00 05 16.61400 +37 37 23.2493           T9 20 0
2 WISEP J031325.96+780744.2 BD* 03 13 25.80778 +78 07 43.8415           T8.5 22 0
3 WISE J033605.05-014350.4 BD* 03 36 05.24056 -01 43 38.7643           Y0 22 0
4 WISE J035000.32-565830.2 BD* 03 50 00.59649 -56 58 24.2429           Y1 35 0
5 WISE J041022.71+150248.4 BD* 04 10 22.07612 +15 03 10.9840           Y0 45 0
6 2MASSI J0415195-093506 BD* 04 15 19.54368 -09 35 06.6732           T8.0 182 0
7 WISE J045853.89+643452.5 BD* 04 58 53.57916 +64 34 49.5816           T8.5 32 0
8 WISE J064723.23-623235.5 BD* 06 47 23.22644 -62 32 39.7006           Y1 24 0
9 WISE J072227.27-054029.9 BD* 07 22 27.9060 -05 40 33.577           T9 90 0
10 WISEA J085510.74-071442.5 BD* 08 55 16.53798 -07 14 49.3728           Y2 124 0
11 2MASS J11101001+0116130 BD* 11 10 10.01064 +01 16 13.0872           T5.5 86 0
12 WISE J121756.90+162640.8 BD* 12 17 56.35451 +16 26 53.6955           T9+Y0 51 0
13 WISE J140518.39+553421.3 BD* 14 05 21.24937 +55 34 18.8785           Y0(pec?) 66 0
14 WISE J205628.91+145953.2 BD* 20 56 28.31061 +14 59 47.8010           Y0 58 0
15 Wolf 940 B BD* 21 46 38.4345 -00 10 34.714           T8.5 62 0
16 WISEA J235402.79+024014.1 BD* 23 54 02.41845 +02 40 18.5413           Y1 18 0

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