2010ApJ...723..850B


Query : 2010ApJ...723..850B

2010ApJ...723..850B - Astrophys. J., 723, 850-868 (2010/November-1)

Near-infrared spectroscopy of the extrasolar planet HR 8799 b.

BOWLER B.P., LIU M.C., DUPUY T.J. and CUSHING M.C.

Abstract (from CDS):

We present 2.12-2.23 µm high contrast integral field spectroscopy of the extrasolar planet HR 8799 b. Our observations were obtained with OSIRIS on the Keck II telescope and sample the 2.2 µm CH4feature, which is useful for spectral classification and as a temperature diagnostic for ultracool objects. The spectrum of HR 8799 b is relatively featureless, with little or no methane absorption, and does not exhibit the strong CH4 seen in T dwarfs of similar absolute magnitudes. The spectrum is consistent with field objects from early-L to T4 (3σ confidence level), with a best-fitting type of T2. A similar analysis of the published 1-4 µm photometry shows the infrared spectral energy distribution (SED) matches L5-L8 field dwarfs, especially the reddest known objects which are believed to be young and/or very dusty. Overall, we find that HR 8799 b has a spectral type consistent with L5-T2, although its SED is atypical compared to most field objects. We fit the 2.2 µm spectrum and the infrared SED using the Hubeny & Burrows, Burrows et al., and Ames-Dusty model atmosphere grids, which incorporate non-equilibrium chemistry, non-solar metallicities, and clear and cloudy variants. No models agree with all of the data, but those with intermediate clouds produce significantly better fits. The largest discrepancy occurs in the J band, which is highly suppressed in HR 8799 b. Models with high eddy diffusion coefficients and high metallicities are somewhat preferred over those with equilibrium chemistry and solar metallicity. The best-fitting effective temperatures range from 1300 to 1700 K with radii between ∼0.3 and 0.5 RJup. These values are inconsistent with evolutionary model-derived values of 800-900 K and 1.1-1.3 RJup based on the luminosity of HR 8799 b and the age of HR 8799, a discrepancy that probably results from imperfect atmospheric models or the limited range of physical parameters covered by the models. The low temperature inferred from evolutionary models indicates that HR 8799 b is ∼400 K cooler than field L/T transition objects, providing further evidence that the L/T transition is gravity-dependent. With an unusually dusty photosphere, an exceptionally low luminosity for its spectral type, and hints of extreme secondary physical parameters, HR 8799 b appears to be unlike any class of field brown dwarf currently known.

Abstract Copyright: ∼

Journal keyword(s): planetary systems - stars: individual: HR 8799 - techniques: image processing

Simbad objects: 37

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Number of rows : 37
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 NAME THA MGr 00 00 -62.0           ~ 540 0
2 2MASS J01075242+0041563 BD* 01 07 52.42200 +00 41 56.3964           L8 64 0
3 SIPS J0227-1624 BD* 02 27 10.3319565862 -16 24 47.668301470         16.846 L1.5 33 0
4 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
5 2MASSI J0415195-093506 BD* 04 15 19.54368 -09 35 06.6732           T8.0 182 0
6 * bet Pic PM* 05 47 17.0876901 -51 03 59.441135 4.13 4.03 3.86 3.74 3.58 A6V 2087 1
7 HD 44627B BD* 06 19 12.9988086984 -58 03 20.198341332           L1 155 1
8 2MASSI J0755480+221218 BD* 07 55 47.95488 +22 12 16.9416           T5.2 37 0
9 2MASS J07584037+3247245 BD* 07 58 40.3517739525 +32 47 23.984796389           T0.0+T3.5 54 0
10 2MASSI J0825196+211552 BD* 08 25 19.6125672818 +21 15 51.549358145       21.97 19.22 L7.5V 138 0
11 2MASS J08575849+5708514 BD* 08 57 58.4721442289 +57 08 51.414025854           L7V 57 0
12 2MASSI J1010148-040649 BD* 10 10 14.80704 -04 06 49.9320           L6 73 0
13 2MASSW J1036530-344138 BD* 10 36 53.0605368096 -34 41 38.377435973           L6 30 0
14 NAME TW Hya Association As* 11 01.9 -34 42           ~ 1018 0
15 TWA 27 LM* 12 07 33.4675524840 -39 32 54.016625184     19.95 17.99 15.88 M8IVe 376 0
16 TWA 27B BD* 12 07 33.50 -39 32 54.4           L3 321 0
17 SDSS J120747.17+024424.8 BD* 12 07 47.17392 +02 44 24.9288           L6.5+T2.5 73 0
18 * lam Boo dS* 14 16 23.0184083839 +46 05 17.895459693 4.31 4.26 4.18 4.16 4.13 A0Va_lB 362 0
19 SDSS J143553.24+112948.5 BD* 14 35 53.341920 +11 29 49.91496           L7.5+T6.0 14 0
20 2MASS J15031961+2525196 BD* 15 03 19.6109033841 +25 25 19.795679019           T5.5 84 0
21 * eta CrB C BD* 15 23 22.63488 +30 14 56.2092           L8V 118 1
22 V* GQ Lup B LM* 15 49 12.05 -35 39 05.1           M9e 165 1
23 RX J1609.5-2105 Or* 16 09 30.3075290712 -21 04 58.943800992   14.21 12.77 12.25 10.99 M0.0e 103 0
24 RX J1609.5-2105B LM* 16 09 30.377 -21 04 56.97           ~ 123 0
25 2MASS J16173168+4019003 BD* 16 17 31.68864 +40 19 00.3684           L6.5 9 0
26 2MASS J16322911+1904407 BD* 16 32 29.11416 +19 04 40.7136       22.42 19.98 L8V 145 0
27 HD 203030 BY* 21 18 58.2195697224 +26 13 49.960929036   9.206 8.426 8.79   K0V 102 0
28 HD 203030B BD* 21 18 58.97 +26 13 46.1           L7.5 77 0
29 2MASSW J2148162+400359 BD* 21 48 16.2986589335 +40 03 59.331851811           L7 80 0
30 HD 208108 * 21 53 37.3886477424 +19 40 06.479949432   5.693 5.676     A0Vs 69 0
31 2MASS J22443167+2043433 BD* 22 44 31.67376 +20 43 43.3020           L6-L8gamma 114 0
32 2MASS J22495345+0044046 BD* 22 49 53.45592 +00 44 04.6608           L3+L5 49 0
33 * alf PsA PM* 22 57 39.04625 -29 37 20.0533 1.31 1.25 1.16 1.11 1.09 A4V 1303 3
34 HD 218396b Pl 23 07 28.7157209544 +21 08 03.310767492           ~ 323 1
35 HD 218396c Pl 23 07 28.7157209544 +21 08 03.310767492           ~ 312 1
36 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0
37 2MASS J23312378-4718274 BD* 23 31 23.78712 -47 18 27.4356           T5 25 0

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