3.8 μm Imaging of 400–600 K Brown Dwarfs and Orbital Constraints for WISEP J045853.90+643452.6AB
Half of the energy emitted by late-T- and Y-type brown dwarfs emerges at 3.5 ≤ λ μ m ≤ 5.5. We present new L ′ (3.43 ≤ λ μ m ≤ 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...
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Veröffentlicht in: | The Astrophysical journal 2019-09, Vol.882 (2), p.117 |
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Hauptverfasser: | , , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Half of the energy emitted by late-T- and Y-type brown dwarfs emerges at 3.5 ≤
λ
μ
m ≤ 5.5. We present new
L
′ (3.43 ≤
λ
μ
m ≤ 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
μ
m 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
T
eff
= 500 K and ∼4 at
T
eff
= 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. |
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ISSN: | 0004-637X 1538-4357 |
DOI: | 10.3847/1538-4357/ab3393 |