2003ApJ...596..561M


Query : 2003ApJ...596..561M

2003ApJ...596..561M - Astrophys. J., 596, 561-586 (2003/October-2)

The NIRSPEC Brown Dwarf Spectroscopic Survey. I. Low-resolution near-infrared spectra.

McLEAN I.S., McGOVERN M.R., BURGASSER A.J., KIRKPATRICK J.D., PRATO L. and KIM S.S.

Abstract (from CDS):

We present the first results of a near-infrared (0.96-2.31 µm) spectroscopic survey of M, L, and T dwarfs obtained with NIRSPEC on the Keck II telescope. Our new survey has a resolving power of R=λ/Δλ∼2000 and is comprised of two major data sets: 53 J-band (1.14-1.36 µm) spectra covering all spectral types from M6 to T8 with at least two members in each spectral subclass (wherever possible), and 25 flux-calibrated spectra from 1.14 to 2.31 µm for most spectral classes between M6 and T8. Sixteen of these 25 objects have additional spectral coverage from 0.96 to 1.14 µm to provide overlap with optical spectra. Spectral flux ratio indexes for prominent molecular bands are derived, and equivalent widths (EWs) for several atomic lines are measured. We find that a combination of four H2O and two CH4 band strengths can be used for spectral classification of all these sources in the near-infrared and that the H2O indexes are almost linear with spectral type from M6 to T8. The H2O indexes near 1.79 and 1.96 µm should remain useful beyond T8. In the near-infrared a notable feature at the boundary between the M and L types is the disappearance of relatively weak (EW∼1-2 Å) atomic lines of Al I and Ca I, followed by Fe I around L2. At the boundary between L and T dwarfs it is the appearance of CH4in all near-infrared bands (J, H, and K) that provides a significant spectral change, although we find evidence of CH4as early as L7 in the K band. The FeH strength and the equivalent width of the K I lines are not monotonic, but in combination with other factors provide useful constraints on spectral type. The K I lines are sensitive to surface gravity. The CO band strength near 2.30 µm is relatively insensitive to spectral class. The peak calibrated flux (Fλ) in the 0.96-2.31 µm region occurs near 1.10 µm at M6 but shifts to about 1.27 µm at T8. In addition, the relative peak flux in the J, H, and K bands is always in the sense J>H>K except around L6, where the differences are small. One object, 2MASS 2244+20 (L6.5), shows normal spectral behavior in the optical but has an infrared spectrum in which the peak flux in J band is less than at H and K.

Abstract Copyright: ∼

Journal keyword(s): Infrared: Stars - Stars: Low-Mass, Brown Dwarfs - Surveys - Techniques: Spectroscopic

Simbad objects: 55

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Number of rows : 55
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 J0015447+351603 BD* 00 15 44.7745521624 +35 16 02.641954548           L1.0V 49 0
2 LSPM J0036+1821 BD* 00 36 16.1118891182 +18 21 10.286665966       18.451 16.053 L3.5 230 0
3 2MASSI J0103320+193536 BD* 01 03 32.03712 +19 35 36.1824           L6V 93 0
4 BRLT 38 BD* 01 51 41.55936 +12 44 30.0768           T0.5 74 0
5 DENIS J020529.0-115925 BD* 02 05 29.3651195393 -11 59 29.721210536           L7V 156 0
6 2MASS J02081833+2542533 BD* 02 08 18.3864053730 +25 42 53.199852759           L1V 53 0
7 2MASSW J0310599+164816 BD* 03 10 59.86560 +16 48 15.5988           L8V 57 0
8 LP 412-31 LM* 03 20 59.7114769400 +18 54 22.770750621   20.5 18.881 16.904 14.484 M8V 130 0
9 2MASSI J0328426+230205 BD* 03 28 42.65592 +23 02 05.1900           L9.5 50 0
10 Cl* Melotte 22 KPNO 2 BD* 03 45 43.1616128256 +25 40 23.239779672         17.36 L0V 136 0
11 2MASSI J0415195-093506 BD* 04 15 19.54368 -09 35 06.6732           T8.0 182 0
12 2MASSI J0423485-041403 BD* 04 23 48.5763811987 -04 14 03.246502948           L6.5+T2 137 0
13 2MASS J05591914-1404488 BD* 05 59 19.1872549354 -14 04 49.206913185           T4.5 159 0
14 HD 42581B BD* 06 10 34.80 -21 52 00.0           T6.5 549 0
15 2MASSI J0727182+171001 BD* 07 27 18.24600 +17 10 01.2072           T7.0 104 0
16 LP 783-2 PM* 07 40 19.3718248157 -17 24 45.912945536   17.6 16.696 14.695 12.37 M6.5Ve 98 0
17 LSPM J0746+2000 BD* 07 46 42.56207 +20 00 32.1839       17.9 15.034 L0+L1.5 201 1
18 SDSS J083717.21-000018.0 BD* 08 37 17.192664 -00 00 20.67084           T1 57 0
19 2MASS J08503593+1057156 BD* 08 50 35.93400 +10 57 15.6168       22.466 20.349 L6.5+L8.5 85 0
20 LP 666-9 BD* 08 53 36.1604798120 -03 29 32.197505547     18.959 16.781 14.487 M9Ve 274 1
21 * pi.01 Cnc C BD* 09 12 14.69112 +14 59 39.6240           L8.5+L7.5 61 1
22 2MASS J09261537+5847212 BD* 09 26 15.37752 +58 47 21.2280           T3.5+T5 39 0
23 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 79 0
24 HD 89744B BD* 10 22 14.8720836024 +41 14 26.514370356           L0.5 50 0
25 2MASSW J1035246+250745 BD* 10 35 24.5190408172 +25 07 44.589716437           L1V 24 0
26 Wolf 359 PM* 10 56 28.9208702274 +07 00 53.003285286 16.706 15.541 13.507 11.684 9.507 dM6 775 0
27 LP 551-63 PM* 11 06 18.9746601198 +04 28 32.670142533   20.2 19.560 17.25 14.91 M6.5V 39 0
28 SIPS J1228-1547 BD* 12 28 15.23184 -15 47 34.2312       20.414 18.042 L5.5+L5.5 151 0
29 2MASS J12373919+6526148 BD* 12 37 39.19632 +65 26 14.8092           T6.5 85 0
30 2MASS J12391934+2029519 LM* 12 39 19.3566181176 +20 29 51.905452092           M9V 12 0
31 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 167 0
32 2MASSI J1300425+191235 BD* 13 00 42.5082106014 +19 12 34.598653499         15.9 L1.7V 64 0
33 NAME Kelu-1 BD* 13 05 40.1642434199 -25 41 05.712165150         16.85 L2+L3.5 267 0
34 GD 165B BD* 14 24 39.09480 +09 17 10.4352         20.53 L4V 216 0
35 GD 165 WD* 14 24 39.1495824408 +09 17 14.160753960   14.46 14.32 14.6 14.91 DA4.1 176 0
36 2MASS J14392836+1929149 BD* 14 39 28.1499428599 +19 29 15.908790370           L1V 145 0
37 GJ 570 D BD* 14 57 14.96256 -21 21 47.7504           T8 242 1
38 2MASSW J1506544+132106 BD* 15 06 54.3299045806 +13 21 06.039351151           L3 116 0
39 2MASSW J1507476-162738 BD* 15 07 47.6758255542 -16 27 40.113982846     22.136 18.928 16.579 L5V 216 0
40 * eta CrB C BD* 15 23 22.63488 +30 14 56.2092           L8V 118 1
41 2MASS J15530228+1532369 BD* 15 53 02.28072 +15 32 36.9132           T6.5+T7.5 63 0
42 2MASSW J1615441+355900 BD* 16 15 44.1554776882 +35 58 59.573277980           L3V 45 0
43 2MASS J16241436+0029158 BD* 16 24 14.36712 +00 29 15.8172           T6V 162 0
44 2MASS J16322911+1904407 BD* 16 32 29.11416 +19 04 40.7136       22.42 19.98 L8V 145 0
45 VB 8 LM* 16 55 35.2557374336 -08 23 40.753073075   18.7 16.916 14.566 12.24 M7Ve 457 0
46 LSPM J1658+7027 BD* 16 58 03.8028228991 +70 27 01.695233449       19.0   L1(e) 44 0
47 2MASSI J1726000+153819 BD* 17 26 00.07752 +15 38 19.0140           L2V 49 0
48 2MASSW J1728114+394859 BD* 17 28 11.50056 +39 48 59.3100           L5+L6.5 65 0
49 2MASS J17503293+1759042 BD* 17 50 32.93832 +17 59 04.2504           T3.5 56 0
50 VB 10 PM* 19 16 57.6109547886 +05 09 01.600923413     17.30     M8V 499 1
51 SIPS J2130-0845 BD* 21 30 44.6489028062 -08 45 20.574092550       19.784 17.351 L1 51 1
52 2MASSI J2158045-155009 BD* 21 58 04.5716969232 -15 50 09.793729140       20.771 18.582 L4 59 0
53 2MASS J22443167+2043433 BD* 22 44 31.67376 +20 43 43.3020           L6-L8gamma 114 0
54 2MASSI J2254188+312349 BD* 22 54 18.92016 +31 23 49.8300           T5.0 80 0
55 2MASSI J2356547-155310 BD* 23 56 54.77040 -15 53 11.1336           T5.8 48 0

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