2004PASP..116....9S


Query : 2004PASP..116....9S

2004PASP..116....9S - Publ. Astron. Soc. Pac., 116, 9-21 (2004/January-0)

JHK magnitudes for L and T dwarfs and infrared photometric systems.

STEPHENS D.C. and LEGGETT S.K.

Abstract (from CDS):

In the last few years a significant population of ultracool L and T dwarfs has been discovered. With effective temperatures ranging from ∼2200 to 700 K, these objects emit most of their radiation in the near-IR, and their spectral energy distributions are dominated by strong molecular absorption bands. These highly structured energy distributions lead to JHK magnitudes that are extremely sensitive to the exact filter bandpass used. In the case of the T dwarfs, the differences between commonly used photometric systems can be as large as 0.4 mag at J and 0.5 mag at J-K. Near-IR magnitudes have been published for L and T dwarfs using a variety of photometric systems. Currently, the data obtained with these systems cannot be accurately compared or combined, as transformations based on the colors of hotter stars are not valid for L and T dwarfs. To address this problem, we have synthesized J, H, and K magnitudes for some of the common photometric systems and present transformation equations with respect to the most atmospheric-independent system, the Mauna Kea Observatory filter set. If the spectral type of the dwarf is known, our transformations allow data to be converted between systems to 0.01 mag, which is better than the typical measurement uncertainty. Transforming on the basis of color alone is more difficult because of the degeneracy and intrinsic scatter in the near-IR colors of L and T dwarfs; in this case J magnitudes can only be transformed to ≲0.05 mag and H and K to ≲0.02 mag.

Abstract Copyright:

Journal keyword(s): Methods: Data Analysis - Stars: Fundamental Parameters - Stars: Low-Mass, Brown Dwarfs

CDS comments: Table 1 : Several SDSS and 2MASS not identified, incomplete format.

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 2MASSI J0028394+150141 BD* 00 28 39.43224 +15 01 41.8620           L4.5V 21 0
2 LSPM J0036+1821 BD* 00 36 16.1118891182 +18 21 10.286665966       18.451 16.053 L3.5 213 0
3 DENIS J020529.0-115925 BD* 02 05 29.3651195393 -11 59 29.721210536           L7V 150 0
4 2MASSW J0310599+164816 BD* 03 10 59.86560 +16 48 15.5988           L8V 49 0
5 2MASSI J0328426+230205 BD* 03 28 42.65592 +23 02 05.1900           L9.5 47 0
6 2MASS J04150289-0859577 * 04 15 02.8926941808 -08 59 57.751470816   17.30       ~ 1 2
7 SIPS J0539-0059 BD* 05 39 52.0040375405 -00 59 01.491092352           L5V 88 0
8 2MASS J05591914-1404488 BD* 05 59 19.1872549354 -14 04 49.206913185           T4.5 150 0
9 HD 42581B BD* 06 10 34.80 -21 52 00.0           T6.5 504 0
10 LSPM J0746+2000 BD* 07 46 42.50553 +20 00 31.9757       17.9 15.034 L0+L1.5 184 1
11 2MASSI J0825196+211552 BD* 08 25 19.6125672818 +21 15 51.549358145       21.97 19.22 L7.5V 123 0
12 SDSS J083717.21-000018.0 BD* 08 37 17.20032 -00 00 19.3608           T1 51 0
13 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 75 0
14 2MASS J12171110-0311131 BD* 12 17 11.10288 -03 11 13.1748           T7.5 85 0
15 2MASS J12255432-2739466 BD* 12 25 54.32328 -27 39 46.6776           T5.5+T8 61 0
16 SIPS J1228-1547 BD* 12 28 15.23184 -15 47 34.2312       20.187 18.163 L5.5+L5.5 145 0
17 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 150 0
18 NAME Kelu-1 BD* 13 05 40.1642434199 -25 41 05.712165150         16.85 L2+L3.5 254 0
19 2MASS J13262981-0038314 BD* 13 26 29.81880 -00 38 31.4880           L5.5V 41 0
20 2MASS J13464634-0031501 BD* 13 46 46.34496 -00 31 50.1312           T6 75 0
21 GD 165B BD* 14 24 39.09480 +09 17 10.4352         20.53 L4V 205 0
22 GJ 570 D BD* 14 57 14.96256 -21 21 47.7504           T8 225 1
23 * eta CrB C BD* 15 23 22.63488 +30 14 56.2092           L8V 105 1
24 2MASS J16322911+1904407 BD* 16 32 29.11416 +19 04 40.7136       22.42 19.98 L8V 131 0

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