2014ApJ...793...75R


Query : 2014ApJ...793...75R

2014ApJ...793...75R - Astrophys. J., 793, 75 (2014/October-1)

Strong brightness variations signal cloudy-to-clear transition of brown dwarfs.

RADIGAN J., LAFRENIERE D., JAYAWARDHANA R. and ARTIGAU E.

Abstract (from CDS):

We report the results of a J-band search for cloud-related variability in the atmospheres of 62 L4-T9 dwarfs using the Du Pont 2.5 m telescope at Las Campanas Observatory and the Canada-France-Hawaii Telescope on Mauna Kea. We find 9 of 57 objects included in our final analysis to be significantly variable with >99% confidence, 5 of which are new discoveries. In our study, strong signals (peak-to-peak amplitudes >2%) are confined to the L/T transition (4/16 objects with L9-T3.5 spectral types and 0/41 objects for all other spectral types). The probability that the observed occurrence rates for strong variability inside and outside the L/T transition originate from the same underlying true occurrence rate is excluded at >99.7% confidence. Based on a careful assessment of our sensitivity to astrophysical signals, we infer that 39–14+16 % of L9-T3.5 dwarfs are strong variables on rotational timescales. If we consider only L9-T3.5 dwarfs with 0.8 < J - Ks< 1.5, and assume an isotropic distribution of spin axes for our targets, we find that 80–19+18 % would be strong variables if viewed edge-on; azimuthal symmetry and/or binarity may account for non-variable objects in this group. These observations suggest that the settling of condensate clouds below the photosphere in brown dwarf (BD) atmospheres does not occur in a spatially uniform manner. Rather, the formation and sedimentation of dust grains at the L/T transition is coupled to atmospheric dynamics, resulting in highly contrasting regions of thick and thin clouds and/or clearings. Outside the L/T transition we identify five weak variables (peak-to-peak amplitudes of 0.6%-1.6%). Excluding L9-T3.5 spectral types, we infer that 60–8+22% of targets vary with amplitudes of 0.5%-1.6%, suggesting that surface heterogeneities are common among L and T dwarfs. Our survey establishes a significant link between strong variability and L/T transition spectral types, providing evidence in support of the hypothesis that cloud holes contribute to the abrupt decline in condensate opacity and 1 µm brightening observed in this regime. More generally, fractional cloud coverage is an important model parameter for BDs and giant planets, especially those with L/T transition spectral types and colors.

Abstract Copyright: ∼

Journal keyword(s): brown dwarfs - stars: variables: general

Simbad objects: 66

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Number of rows : 66
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 2MASSW J0030300-145033 BD* 00 30 30.13224 -14 50 33.3960           L7V 52 0
2 2MASS J00501994-3322402 BD* 00 50 19.94352 -33 22 40.2708           T7 45 0
3 SIMP J013656.5+093347.3 BD* 01 36 56.5605419830 +09 33 47.311965969           T2.0 167 0
4 BRLT 38 BD* 01 51 41.55936 +12 44 30.0768           T0.5 74 0
5 2MASS J02074284+0000564 BD* 02 07 42.84984 +00 00 56.4408           T4.5 46 0
6 2MASS J02431371-2453298 BD* 02 43 13.71792 -24 53 29.8356           T6.0 55 0
7 2MASS J02572581-3105523 BD* 02 57 25.8358051304 -31 05 52.195773867           L8.5 40 0
8 2MASSI J0318540-342129 BD* 03 18 54.0760885341 -34 21 29.084072887           L7 33 0
9 2MASSI J0328426+230205 BD* 03 28 42.65592 +23 02 05.1900           L9.5 50 0
10 2MASSI J0415195-093506 BD* 04 15 19.54368 -09 35 06.6732           T8.0 182 0
11 2MASSI J0423485-041403 BD* 04 23 48.5763811987 -04 14 03.246502948           L6.5+T2 137 0
12 2MASS J05103524-4208146 BD* 05 10 35.24352 -42 08 14.6580           T5 14 1
13 2MASS J05160945-0445499 BD* 05 16 09.45840 -04 45 49.9392           T5.5 29 0
14 2MASS J05185995-2828372 BD* 05 18 59.95656 -28 28 37.2720           L6+T4 41 0
15 SIPS J0539-0059 BD* 05 39 52.0040375405 -00 59 01.491092352           L5V 95 0
16 2MASS J05591914-1404488 BD* 05 59 19.1872549354 -14 04 49.206913185           T4.5 159 0
17 2MASS J07222760-0540384 * 07 22 27.6018952248 -05 40 38.348869980           ~ 3 0
18 WISE J072227.27-054029.9 BD* 07 22 27.9060 -05 40 33.577           T9 90 0
19 2MASS J07290002-3954043 BD* 07 29 00.02496 -39 54 04.3992           T8pec 36 0
20 2MASS J07420130+2055198 BD* 07 42 01.30152 +20 55 19.8840           T5 22 0
21 2MASS J07584037+3247245 BD* 07 58 40.3517739525 +32 47 23.984796389           T0.0+T3.5 54 0
22 2MASS J08173001-6155158 BD* 08 17 29.9988806950 -61 55 15.658625335           T6 40 0
23 2MASS J08304878+0128311 BD* 08 30 48.78360 +01 28 31.1520           T5.5 24 0
24 2MASS J09310955+0327331 BD* 09 31 09.55248 +03 27 33.1272           L7.5 12 0
25 2MASS J09393548-2448279 BD* 09 39 35.48976 -24 48 27.9432           T8 69 0
26 2MASS J09490860-1545485 BD* 09 49 08.60280 -15 45 48.5244           T1.0+T2.0 26 0
27 2MASS J10073369-4555147 BD* 10 07 33.69888 -45 55 14.7108           T5 17 0
28 2MASSW J1036530-344138 BD* 10 36 53.0605368096 -34 41 38.377435973           L6 30 0
29 2MASS J10482926+0919373 BD* 10 48 29.26296 +09 19 37.3872           T2.5 16 0
30 2MASS J10521350+4422559 BD* 10 52 13.50504 +44 22 55.9128           L6.5+T1.5 38 0
31 2MASS J11101001+0116130 BD* 11 10 10.01064 +01 16 13.0872           T5.5 86 0
32 2MASS J11145133-2618235 BD* 11 14 51.33720 -26 18 23.5620           T7.5 50 0
33 2MASS J11220826-3512363 BD* 11 22 08.2584613608 -35 12 36.580608360           T2.0 28 0
34 DENIS J112639.9-500355 BD* 11 26 39.8047127039 -50 03 54.846166563         17.800 L5.5 52 0
35 2MASS J11555389+0559577 BD* 11 55 53.89032 +05 59 57.7032           L7.5 39 0
36 TWA 27B BD* 12 07 33.50 -39 32 54.4           L3 321 0
37 SDSS J120747.17+024424.8 BD* 12 07 47.17392 +02 44 24.9288           L6.5+T2.5 73 0
38 2MASS J12095613-1004008 BD* 12 09 56.13096 -10 04 00.8076           T2+T7.5 67 0
39 2MASS J12154430-3420594 BD* 12 15 44.30544 -34 20 59.4600           T4.5 10 0
40 2MASS J12171110-0311131 BD* 12 17 11.10288 -03 11 13.1748           T7.5 92 0
41 ULAS2MASS J1231+0847 BD* 12 31 47.53608 +08 47 33.1116           T6 37 0
42 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 167 0
43 2MASS J13262981-0038314 BD* 13 26 29.81880 -00 38 31.4880           L5.5V 48 0
44 2MASS J14025564+0800553 BD* 14 02 55.64328 +08 00 55.3248           L8+T5? 13 0
45 2MASS J14044948-3159330 BD* 14 04 49.48416 -31 59 33.0576           T1+T5 35 1
46 2MASS J14162408+1348263 BD* 14 16 24.0739698960 +13 48 26.193281184           L5 88 1
47 2MASS J14252798-3650229 BD* 14 25 27.9845344257 -36 50 23.248617541           L4 61 1
48 2MASSW J1507476-162738 BD* 15 07 47.6758255542 -16 27 40.113982846     22.136 18.928 16.579 L5V 216 0
49 SDSS J151114.65+060742.9 BD* 15 11 14.66280 +06 07 43.1652           T2.0 40 0
50 2MASS J15210327+0131426 BD* 15 21 03.27096 +01 31 42.6900           T1+T4 30 0
51 2MASSI J1546271-332511 BD* 15 46 27.18600 -33 25 11.1828           T5.7 34 1
52 2MASS J16241436+0029158 BD* 16 24 14.36712 +00 29 15.8172           T6V 162 0
53 2MASS J16291840+0335371 BD* 16 29 18.40896 +03 35 37.1040           T2 34 0
54 2MASS J16335933-0640552 BD* 16 33 59.33184 -06 40 55.2396           L5.5 15 0
55 2MASS J17054834-0516462 BD* 17 05 48.3505962528 -05 16 46.349087556         16.55 L1 55 1
56 2MASS J17502385+4222373 BD* 17 50 23.85336 +42 22 37.3476           T1 24 0
57 2MASS J17502484-0016151 BD* 17 50 24.8108937456 -00 16 14.995437500       19.98 17.33 L5.5 53 0
58 2MASS J18283572-4849046 BD* 18 28 35.72256 -48 49 04.6380           T6 31 0
59 SIPS J1936-5502 BD* 19 36 01.8856788584 -55 02 32.189687017           L4 22 0
60 SDSS J205235.31-160929.8 BD* 20 52 35.31672 -16 09 29.8620           L8.5+T1.5 23 0
61 CFBDS J213926+022023 BD* 21 39 26.76936 +02 20 22.6968           L8.5+T3.5 108 0
62 2MASS J21513839-4853542 BD* 21 51 38.39304 -48 53 54.2508           T4.5 21 0
63 2MASS J22282889-4310262 BD* 22 28 28.89432 -43 10 26.2740           T6.5 74 0
64 2MASSI J2254188+312349 BD* 22 54 18.92016 +31 23 49.8300           T5.0 80 0
65 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0
66 2MASS J23312378-4718274 BD* 23 31 23.78712 -47 18 27.4356           T5 25 0

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