2004AJ....127.3516G


Query : 2004AJ....127.3516G

2004AJ....127.3516G - Astron. J., 127, 3516-3536 (2004/June-0)

L' and M' photometry of ultracool dwarfs.

GOLIMOWSKI D.A., LEGGETT S.K., MARLEY M.S., FAN X., GEBALLE T.R., KNAPP G.R., VRBA F.J., HENDEN A.A., LUGINBUHL C.B., GUETTER H.H., MUNN J.A., CANZIAN B., ZHENG W., TSVETANOV Z.I., CHIU K., GLAZEBROOK K., HOVERSTEN E.A., SCHNEIDER D.P. and BRINKMANN J.

Abstract (from CDS):

We have compiled L' (3.4-4.1 µm) and M' (4.6-4.8 µm) photometry of 63 single and binary M, L, and T dwarfs obtained at the United Kingdom Infrared Telescope using the Mauna Kea Observatory filter set. This compilation includes new L' measurements of eight L dwarfs and 13 T dwarfs and new M' measurements of seven L dwarfs, five T dwarfs, and the M1 dwarf Gl 229A. These new data increase by factors of 0.6 and 1.6, respectively, the numbers of ultracool dwarfs (Teff≲2400 K) for which L' and M' measurements have been reported. We compute Lbol, BCK, and Tefffor 42 dwarfs whose flux-calibrated JHK spectra, L' photometry, and trigonometric parallaxes are available, and we estimate these quantities for nine other dwarfs whose parallaxes and flux-calibrated spectra have been obtained. BCKis a well-behaved function of near-infrared spectral type with a dispersion of ∼0.1 mag for types M6-T5; it is significantly more scattered for types T5-T9. Teff declines steeply and monotonically for types M6-L7 and T4-T9, but it is nearly constant at ∼1450 K for types L7-T4 with assumed ages of ∼3 Gyr. This constant Teffis evidenced by nearly unchanging values of L'-M' between types L6 and T3. It also supports recent models that attribute the changing near-infrared luminosities and spectral features across the L-T transition to the rapid migration, disruption, and/or thinning of condensate clouds over a narrow range of Teff. The L' and M' luminosities of early-T dwarfs do not exhibit the pronounced humps or inflections previously noted in the I through K bands, but insufficient data exist for types L6-T5 to assert that M_L'_and M_M'_are strictly monotonic within this range of types. We compare the observed K, L', and M' luminosities of L and T dwarfs in our sample with those predicted by precipitating-cloud and cloud-free models for varying surface gravities and sedimentation efficiencies. The models indicate that the L3-T4.5 dwarfs generally have higher gravities (logg=5.0-5.5) than the T6-T9 dwarfs (logg=4.5-5.0). The predicted M' luminosities of late-T dwarfs are 1.5-2.5 times larger than those derived empirically for the late-T dwarfs in our sample. This discrepancy is attributed to absorption at 4.5-4.9 µm by CO, which is not expected under the condition of thermochemical equilibrium assumed in the models. Our photometry and bolometric calculations indicate that the L3 dwarf Kelu-1 and the T0 dwarf SDSS J042348.57-041403.5 are probable binary systems. We compute log(Lbol/L)=-5.73±0.05 and Teff=600-750 K for the T9 dwarf 2MASSI J0415195-093506, which supplants Gl 570D as the least luminous and coolest brown dwarf presently known.–

Abstract Copyright:

Journal keyword(s): Stars: Fundamental Parameters - Stars: Late-Type - Stars: Low-Mass, Brown Dwarfs

Simbad objects: 77

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Number of rows : 77
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 NAME L 362-29 BC BD* 00 04 34.8671722377 -40 44 06.463544237       19.61 16.88 L5+L5 111 0
2 L 362-29 PM* 00 04 36.4375346731 -40 44 02.880162313   14.47 12.84 12.525   M4V 79 0
3 V* DY Psc BY* 00 24 24.6317407560 -01 58 19.954412004     19.42 17.301 15.022 M9.5V 210 1
4 LP 349-25 LM* 00 27 56.0057038615 +22 19 32.635434516   18.6   16.0   M8Ve 73 0
5 2MASS J00325937+1410371 BD* 00 32 59.37576 +14 10 37.1136           L8V 28 0
6 LSPM J0036+1821 BD* 00 36 16.1118891182 +18 21 10.286665966       18.451 16.053 L3.5 213 0
7 2MASS J01075242+0041563 BD* 01 07 52.42200 +00 41 56.3964           L8 55 0
8 BRLT 38 BD* 01 51 41.55936 +12 44 30.0768           T0.5 68 0
9 V* TZ Ari Er* 02 00 12.9563198327 +13 03 07.000569241 15.406 14.100 12.298 10.943 9.195 M4.5V 282 0
10 DENIS J020529.0-115925 BD* 02 05 29.3651195393 -11 59 29.721210536           L7V 150 0
11 2MASS J02074284+0000564 BD* 02 07 42.84984 +00 00 56.4408           T4.5 39 0
12 2MASSI J0243137-245329 BD* 02 43 13.71792 -24 53 29.8356           T6.0 50 0
13 2MASSW J0310599+164816 BD* 03 10 59.86560 +16 48 15.5988           L8V 49 0
14 2MASSI J0328426+230205 BD* 03 28 42.65592 +23 02 05.1900           L9.5 47 0
15 Cl* Melotte 22 KPNO 2 BD* 03 45 43.1616128256 +25 40 23.239779672         17.36 L0V 126 0
16 2MASSI J0415195-093506 BD* 04 15 19.54368 -09 35 06.6732           T8.0 165 0
17 2MASSI J0423485-041403 BD* 04 23 48.5763811987 -04 14 03.246502948           L6.5+T2 125 0
18 SIPS J0539-0059 BD* 05 39 52.0040375405 -00 59 01.491092352           L5V 88 0
19 2MASS J05591914-1404488 BD* 05 59 19.1872549354 -14 04 49.206913185           T4.5 150 0
20 HD 42581 Er* 06 10 34.6149358167 -21 51 52.656352926 10.801 9.607 8.125 7.164 6.121 M1V 478 0
21 HD 42581B BD* 06 10 34.80 -21 52 00.0           T6.5 504 0
22 2MASSI J0727182+171001 BD* 07 27 18.24600 +17 10 01.2072           T7.0 91 0
23 LSPM J0746+2000 BD* 07 46 42.50553 +20 00 31.9757       17.9 15.034 L0+L1.5 184 1
24 2MASS J07584037+3247245 BD* 07 58 40.3517739525 +32 47 23.984796389           T0.0+T3.5 45 0
25 2MASS J08053189+4812330 BD* 08 05 31.8496436040 +48 12 33.131831320           L4+T5 42 0
26 2MASSI J0825196+211552 BD* 08 25 19.6125672818 +21 15 51.549358145       21.97 19.22 L7.5V 123 0
27 2MASS J08300825+4828482 BD* 08 30 08.1496038211 +48 28 47.538657498           L9.5 45 0
28 G 252-13 PM* 08 31 30.1192199475 +73 03 45.775727249   14.61   12.5   M4.0V 45 0
29 SDSS J083717.21-000018.0 BD* 08 37 17.20032 -00 00 19.3608           T1 51 0
30 2MASS J08503593+1057156 BD* 08 50 35.93400 +10 57 15.6168       22.466 20.349 L6.5+L8.5 78 0
31 LP 666-9 LM* 08 53 36.1604798120 -03 29 32.197505547     18.959 16.781 14.487 M9Ve 252 0
32 2MASS J08575849+5708514 BD* 08 57 58.4721442289 +57 08 51.414025854           L7V 47 0
33 2MASS J09083803+5032088 BD* 09 08 38.0091771633 +50 32 08.205341214           L8 46 0
34 * pi.01 Cnc C BD* 09 12 14.69112 +14 59 39.6240           L8.5+L7.5 56 1
35 2MASSI J0937347+293142 BD* 09 37 34.87968 +29 31 40.9908           T6 89 0
36 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 75 0
37 2MASSW J1047539+212423 BD* 10 47 53.85456 +21 24 23.4684           T6.5 86 0
38 LP 731-58 Er* 10 48 12.6142508200 -11 20 09.610693470     15.784 16.01 11.25 M6.5V 174 0
39 Wolf 359 Er* 10 56 28.9208702274 +07 00 53.003285286 16.706 15.541 13.507 11.684 9.507 dM6 721 0
40 SIPS J1058-1548 BD* 10 58 47.8366017792 -15 48 17.250428304       20.095 17.764 L3V 100 2
41 LP 732-94 LM* 11 21 49.1708652037 -13 13 08.693807585     19.57     M8.5V 131 0
42 Ross 128 Er* 11 47 44.3972681420 +00 48 16.400337591 14.223 12.905 11.153 9.859 8.184 dM4 420 0
43 2MASS J12074717+0244249 BD* 12 07 47.17296 +02 44 24.9576           L6.5+T2.5 66 0
44 2MASS J12171110-0311131 BD* 12 17 11.10288 -03 11 13.1748           T7.5 85 0
45 2MASS J12255432-2739466 BD* 12 25 54.32328 -27 39 46.6776           T5.5+T8 61 0
46 SIPS J1228-1547 BD* 12 28 15.23184 -15 47 34.2312       20.187 18.163 L5.5+L5.5 145 0
47 ULAS2MASS J1231+0847 BD* 12 31 47.53608 +08 47 33.1116           T6 34 0
48 Wolf 424 ** 12 33 17.361480 +09 01 15.79224 15.398 14.313 12.467 10.937 8.988 M5.5V 321 0
49 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 150 0
50 NAME Kelu-1 BD* 13 05 40.1642434199 -25 41 05.712165150         16.85 L2+L3.5 254 0
51 2MASS J13262981-0038314 BD* 13 26 29.81880 -00 38 31.4880           L5.5V 41 0
52 2MASS J13464634-0031501 BD* 13 46 46.34496 -00 31 50.1312           T6 75 0
53 GD 165B BD* 14 24 39.09480 +09 17 10.4352         20.53 L4V 205 0
54 LP 271-25 LM* 14 28 43.2275214164 +33 10 39.259309081   21.2   17.8   M9Ve 250 0
55 2MASS J14392836+1929149 BD* 14 39 28.1499428599 +19 29 15.908790370           L1V 131 0
56 LP 326-21 LM* 14 44 17.1771536455 +30 02 14.229564188   20.0   17.8   M8e 25 0
57 2MASS J14460061+0024519 BD* 14 46 00.61560 +00 24 51.9660           L5V 35 0
58 LP 914-54 Er* 14 56 38.2634715567 -28 09 48.619153485     17.141 14.863 12.433 M7.0Ve 156 0
59 GJ 570 D BD* 14 57 14.96256 -21 21 47.7504           T8 225 1
60 TVLM 513-46 LM* 15 01 08.1864639648 +22 50 02.137869060   21.4 15.09 18.0   M8.5V 166 0
61 2MASS J15031961+2525196 BD* 15 03 19.6109033841 +25 25 19.795679019           T5.5 70 0
62 2MASSW J1507476-162738 BD* 15 07 47.6758255542 -16 27 40.113982846     22.136 18.928 16.579 L5V 199 0
63 * eta CrB C BD* 15 23 22.63488 +30 14 56.2092           L8V 105 1
64 2MASSI J1534498-295227 BD* 15 34 49.84080 -29 52 27.4188           T4.5+T5 66 0
65 2MASS J16241436+0029158 BD* 16 24 14.36712 +00 29 15.8172           T6V 145 0
66 2MASS J16322911+1904407 BD* 16 32 29.11416 +19 04 40.7136       22.42 19.98 L8V 131 0
67 Wolf 629 PM* 16 55 25.2222453644 -08 19 21.296969167 14.691 13.436 11.759 10.574 9.044 M3.5V 219 0
68 2MASS J17503293+1759042 BD* 17 50 32.93832 +17 59 04.2504           T3.5 51 0
69 HD 180617 PM* 19 16 55.2565688720 +05 10 08.040554168 11.768 10.63 9.115 8.076 6.782 M3-V 420 0
70 SDSS J204749.59-071818.2 BD* 20 47 49.59816 -07 18 18.2592           L9.5 16 0
71 Wolf 896 PM* 20 56 46.5969248424 -10 26 54.747253252 14.112 12.999 11.487 10.428 9.106 dM2.5 101 0
72 2MASSW J2224438-015852 BD* 22 24 43.8544128559 -01 58 53.284975671           L4.5V 139 0
73 2MASS J22443167+2043433 BD* 22 44 31.67376 +20 43 43.3020           L6-L8gamma 99 0
74 2MASS J22495345+0044046 BD* 22 49 53.45592 +00 44 04.6608           L3+L5 44 0
75 2MASSI J2254188+312349 BD* 22 54 18.92016 +31 23 49.8300           T5.0 70 0
76 2MASS J22552907-0034336 LM* 22 55 29.0832187176 -00 34 33.656819808     20.26     M8.6V 31 1
77 2MASSI J2356547-155310 BD* 23 56 54.77040 -15 53 11.1336           T5.8 43 0

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