2020A&A...643A..23T


Query : 2020A&A...643A..23T

2020A&A...643A..23T - Astronomy and Astrophysics, volume 643A, 23-23 (2020/11-1)

Rotational spectral modulation of cloudless atmospheres for L/T brown dwarfs and extrasolar giant planets.

TREMBLIN P., PHILLIPS M.W., EMERY A., BARAFFE I., LEW B.W.P., APAI D., BILLER B.A. and BONNEFOY M.

Abstract (from CDS):


Aims. The rotational spectral modulation (spectro-photometric variability) of brown dwarfs is usually interpreted as a sign indicating the presence of inhomogeneous cloud covers in the atmosphere. This paper is aimed at exploring the role of temperature fluctuations in these spectral modulations. These fluctuations could naturally arise in a convective atmosphere impacted by such diabatic processes as complex chemistry, namely, a mechanism recently proposed to explain the L/T transition: CO/CH4 radiative convection.
Methods. After exploring the observed spectral-flux ratios between different objects along the cooling sequence, we used the 1D radiative-convective code ATMO, with ad hoc modifications of the temperature gradient, to model the rotational spectral modulation of 2MASS 1821, 2MASS 0136, and PSO 318.5-22. We also explored the impact of CH4 abundance fluctuations on the spectral modulation of 2MASS 0136.
Results. The spectral-flux ratio of different objects along the cooling sequence and the rotational spectral modulation within individual objects at the L/T transition have similar characteristics. This strongly suggests that the main parameter varying along the cooling sequence, namely, temperature, might play a key role in the rotational spectral modulations at the L/T transition. Modeling the spectral bright-to-faint ratio of the modulation of 2MASS 1821, 2MASS 0136, and PSO 318.5-22 shows that most spectral characteristics can be reproduced by temperature variations alone. Furthermore, the approximately anti-correlated variability between different wavelengths can be easily interpreted as a change in the temperature gradient in the atmosphere, which is a consequence we expect from CO/CH4 radiative convection as an explanation of the L/T transition. The deviation from an exact anti-correlation could then be interpreted as a phase shift similar to the hot-spot shift at different bandpasses in the atmospheres of hot Jupiters.
Conclusions. Our results suggest that the rotational spectral modulation from cloud opacity and temperature variations are degenerate. If the nearly anti-correlated signal between different wavelengths is, indeed, a strong sign of a change in the temperature gradient, the detection of direct cloud spectral signatures, for instance, the silicate absorption feature at 10 µm, would help to confirm the presence of clouds and their contribution to spectral modulations (which does not exclude temperature variations or other mechanisms that may also be at play). Future studies considering the differences in the spectral modulation of objects with and without the silicate absorption feature may give us some insight into how to distinguish cloud-opacity fluctuations from temperature fluctuations.

Abstract Copyright: © P. Tremblin et al. 2020

Journal keyword(s): brown dwarfs - methods: numerical - planets and satellites: atmospheres

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 SIMP J013656.5+093347.3 BD* 01 36 56.5605419830 +09 33 47.311965969           T2.0 122 0
2 2MASS J01550354+0950003 BD* 01 55 03.5501844443 +09 50 00.395365641           L4 17 0
3 2MASS J08350622+1953050 BD* 08 35 06.22944 +19 53 05.0532           L5 37 0
4 2MASS J08583467+3256275 BD* 08 58 34.67184 +32 56 27.5640           T1 22 0
5 2MASS J10101480-0406499 BD* 10 10 14.80704 -04 06 49.9320           L6 56 0
6 NAME Luhman 16B BD* 10 49 14.0744805001 -53 19 05.800116097           T0.5 57 0
7 2MASS J11220826-3512363 BD* 11 22 08.2584613608 -35 12 36.580608360           T2 24 0
8 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 147 0
9 SIPS J1256-1257B BD* 12 56 01.83264 -12 57 27.6912           L8.0 63 0
10 2MASSW J1507476-162738 BD* 15 07 47.6758255542 -16 27 40.113982846     22.136 18.928 16.579 L5V 193 0
11 2MASS J18212815+1414010 BD* 18 21 28.1575343503 +14 14 00.859336631           L5 47 0
12 2MASS J21140802-2251358 BD* 21 14 08.02560 -22 51 35.8380           L7.5 103 0
13 2MASS J22282889-4310262 BD* 22 28 28.89432 -43 10 26.2740           T6.5 65 0
14 NAME Carina-near Moving Group MGr ~ ~           ~ 81 0

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2023.06.03-01:02:28

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