Source | H2O-J | CH4-J | H2O-H | CH4-H | CH4-K | Direct | M1 | M2 |
Spectra smoothed to R =150 | ||||||||
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0.650 (T0.0) | 0.656 (T0.0) | 0.592 (T0.0) | 0.873 (T2.0) | 0.587 (T2.0) | T1.0 | T1.0 | ... |
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0.172 (T6.0) | 0.305 (T6.5) | 0.308 (T5.5) | 0.295 (T6.0) | 0.178 (T5.5) | T6.0 | T6.0 | ... |
Spectra smoothed to R =500 | ||||||||
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0.652 (.../...) | 0.657 (T1.0/T1.5) | 0.589 (T1.0/T0.5) | 0.872 (T2.0/T2.0) | 0.588 (T2.0/T2.0) | T1.0 | T1.5 | T1.5 |
![]() |
0.171 (T6.0/T6.0) | 0.302 (T6.0/T6.0) | 0.303 (T6.0/T6.0) | 0.290 (T6.0/T6.0) | 0.180 (T5.5/T5.5) | T6.0 | T6.0 | T6.0 |
Unsmoothed spectra | ||||||||
![]() |
0.645 | 0.660 | 0.589 | 0.870 | 0.589 | T1.0 | ... | ... |
![]() |
0.171 | 0.307 | 0.299 | 0.287 | 0.178 | T6.0 | ... | ... |
The spectra have been smoothed to two resolutions to emulate the observations of the spectral standard stars defined by Burgasser et al. (2006b).
The indices derived from our unsmoothed data have been included to
quantify the uncertainty when measuring indices from spectra at
different resolutions. M1 refers to method 1 of Burgasser et al.
where the measured spectral indices are compared to that of each of the
standard stars, and M2 refers to their method 2 where the
measured spectral indices are compared to a range of values for each
spectral type. Direct classification compares the overall spectral
shape to the standard star spectra. The spectral type derived from each
index is shown in parentheses after each measurement with only M1 being
defined for a resolution of R=500. The average spectral type
from each method is shown on the right-hand side. Only direct
classification is possible for our unsmoothed spectra. The range of the
H2O-J index is ill-defined for the earliest T dwarfs and is therefore omitted for
Indi Ba.
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