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# %ECSV 0.9 | ||
# --- | ||
# datatype: | ||
# - {name: wavelength, unit: Angstrom, datatype: float64} | ||
# - {name: response, datatype: float64} | ||
# meta: !!omap | ||
# - {band_name: H} | ||
# - {description: 'Instrument: 2MASS Cameras in Mt. Hopkins, AZ, and CTIO, Chile | ||
# | ||
# Determined by: Cohen, Wheaton & Megeath (2003), AJ, 126, 1990 with notes: | ||
# | ||
# "Table 1 - 2MASS Isophotal Bandpasses and Fluxes-for-0-magnitude from Cohen et al. (2003) | ||
# Band Lambda (micron) Bandwidth (micron) Fnu - 0 mag (Jy) Flambda - 0 mag (W cm-2 micron-1) | ||
# J 1.235 0.006 0.162 0.001 1594 27.8 3.129E-13 5.464E-15 | ||
# H 1.662 0.009 0.251 0.002 1024 20.0 1.133E-13 2.212E-15 | ||
# Ks 2.159 0.011 0.262 0.002 666.7 12.6 4.283E-14 8.053E-16 | ||
# | ||
# Figures 1, 2, and 3 present the 2MASS J, H and Ks relative spectral | ||
# response curves (RSRs), peak-normalized to unity. These curves are | ||
# derived by Cohen et al. (2003) and are photon-counting RSRs suitable | ||
# for integrating over stellar spectra when using or generating synthetic | ||
# photometry. These RSRs are consistent with the absolute calibration of | ||
# 2MASS given in Table 1 above." | ||
# | ||
# Notes: | ||
# I am not in a position to judge the quality of these curves, but | ||
# have no reason to doubt them. - Michael Blanton 2005-07-06'} | ||
# - {group_name: twomass} | ||
wavelength response | ||
13000.0 0 | ||
13150.0 0 | ||
13410.0 0 | ||
13680.0 0 | ||
13970.0 0 | ||
14180.0 0 | ||
14400.0 3.47222e-08 | ||
14620.0 1.91518e-07 | ||
14780.0 5.48038e-07 | ||
14860.0 1.93136e-06 | ||
14930.0 5.83389e-06 | ||
15040.0 1.3391e-05 | ||
15150.0 2.89241e-05 | ||
15280.0 4.49215e-05 | ||
15390.0 5.31579e-05 | ||
15460.0 5.70569e-05 | ||
15510.0 5.87879e-05 | ||
15560.0 5.95694e-05 | ||
15650.0 5.93802e-05 | ||
15720.0 5.55153e-05 | ||
15770.0 5.43183e-05 | ||
15830.0 5.57549e-05 | ||
15920.0 5.76696e-05 | ||
15970.0 5.80276e-05 | ||
16020.0 5.66542e-05 | ||
16130.0 5.74086e-05 | ||
16190.0 5.68561e-05 | ||
16280.0 5.6769e-05 | ||
16330.0 5.65524e-05 | ||
16420.0 5.73569e-05 | ||
16480.0 5.7591e-05 | ||
16570.0 5.91853e-05 | ||
16590.0 5.98975e-05 | ||
16710.0 5.98444e-05 | ||
16840.0 5.67755e-05 | ||
17010.0 5.43269e-05 | ||
17150.0 5.72653e-05 | ||
17270.0 5.74175e-05 | ||
17390.0 5.68545e-05 | ||
17460.0 5.60825e-05 | ||
17510.0 5.52941e-05 | ||
17530.0 5.34512e-05 | ||
17560.0 5.23349e-05 | ||
17640.0 4.77494e-05 | ||
17750.0 3.75831e-05 | ||
17850.0 1.50924e-05 | ||
17900.0 2.5229e-05 | ||
17960.0 9.63809e-06 | ||
18030.0 5.97338e-06 | ||
18100.0 3.90608e-06 | ||
18130.0 2.81302e-07 | ||
18180.0 1.10011e-06 | ||
18280.0 2.18818e-08 | ||
18350.0 0 | ||
18500.0 5.40541e-09 | ||
18710.0 0 | ||
18930.0 0 | ||
19150.0 0 |
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@@ -0,0 +1,136 @@ | ||
# %ECSV 0.9 | ||
# --- | ||
# datatype: | ||
# - {name: wavelength, unit: Angstrom, datatype: float64} | ||
# - {name: response, datatype: float64} | ||
# meta: !!omap | ||
# - {band_name: J} | ||
# - {description: 'Instrument: 2MASS Cameras in Mt. Hopkins, AZ, and CTIO, Chile | ||
# | ||
# Determined by: Cohen, Wheaton & Megeath (2003), AJ, 126, 1990 with notes: | ||
# | ||
# "Table 1 - 2MASS Isophotal Bandpasses and Fluxes-for-0-magnitude from Cohen et al. (2003) | ||
# Band Lambda (micron) Bandwidth (micron) Fnu - 0 mag (Jy) Flambda - 0 mag (W cm-2 micron-1) | ||
# J 1.235 0.006 0.162 0.001 1594 27.8 3.129E-13 5.464E-15 | ||
# H 1.662 0.009 0.251 0.002 1024 20.0 1.133E-13 2.212E-15 | ||
# Ks 2.159 0.011 0.262 0.002 666.7 12.6 4.283E-14 8.053E-16 | ||
# | ||
# Figures 1, 2, and 3 present the 2MASS J, H and Ks relative spectral | ||
# response curves (RSRs), peak-normalized to unity. These curves are | ||
# derived by Cohen et al. (2003) and are photon-counting RSRs suitable | ||
# for integrating over stellar spectra when using or generating synthetic | ||
# photometry. These RSRs are consistent with the absolute calibration of | ||
# 2MASS given in Table 1 above." | ||
# | ||
# Notes: | ||
# I am not in a position to judge the quality of these curves, but | ||
# have no reason to doubt them. - Michael Blanton 2005-07-06'} | ||
# - {group_name: twomass} | ||
wavelength response | ||
10620.0 0 | ||
10660.0 4.69043e-08 | ||
10700.0 1.86916e-07 | ||
10750.0 3.16279e-07 | ||
10780.0 6.58627e-07 | ||
10820.0 1.46026e-06 | ||
10840.0 2.41697e-06 | ||
10870.0 3.64305e-06 | ||
10890.0 4.80257e-06 | ||
10930.0 6.08417e-06 | ||
10960.0 6.63321e-06 | ||
11020.0 8.41198e-06 | ||
11050.0 2.47602e-05 | ||
11070.0 3.0804e-05 | ||
11090.0 3.23174e-05 | ||
11120.0 3.41817e-05 | ||
11160.0 2.96326e-05 | ||
11170.0 2.14414e-05 | ||
11200.0 2.1375e-05 | ||
11230.0 2.52271e-05 | ||
11280.0 2.28901e-05 | ||
11290.0 2.22763e-05 | ||
11320.0 4.75353e-05 | ||
11340.0 1.96825e-05 | ||
11380.0 4.71793e-05 | ||
11400.0 9.66667e-06 | ||
11430.0 4.62992e-05 | ||
11470.0 2.28335e-05 | ||
11540.0 2.7747e-05 | ||
11590.0 1.50388e-05 | ||
11640.0 5.21478e-05 | ||
11670.0 5.29477e-05 | ||
11700.0 5.78034e-05 | ||
11730.0 6.20546e-05 | ||
11750.0 6.35319e-05 | ||
11790.0 7.04326e-05 | ||
11820.0 6.68612e-05 | ||
11860.0 6.82631e-05 | ||
11880.0 7.04461e-05 | ||
11920.0 7.01342e-05 | ||
11950.0 6.27531e-05 | ||
11990.0 5.90492e-05 | ||
12020.0 5.81364e-05 | ||
12090.0 5.83044e-05 | ||
12160.0 5.75987e-05 | ||
12210.0 6.00164e-05 | ||
12270.0 5.75143e-05 | ||
12310.0 6.84322e-05 | ||
12360.0 7.45874e-05 | ||
12400.0 7.68145e-05 | ||
12440.0 7.77814e-05 | ||
12470.0 7.69447e-05 | ||
12530.0 7.36393e-05 | ||
12550.0 7.11554e-05 | ||
12580.0 6.77981e-05 | ||
12600.0 6.36746e-05 | ||
12650.0 5.92964e-05 | ||
12700.0 5.33937e-05 | ||
12750.0 5.11686e-05 | ||
12790.0 4.99453e-05 | ||
12860.0 4.99533e-05 | ||
12920.0 5.02012e-05 | ||
12970.0 5.26137e-05 | ||
13020.0 5.78264e-05 | ||
13050.0 5.94559e-05 | ||
13070.0 6.21117e-05 | ||
13100.0 5.9313e-05 | ||
13130.0 5.49124e-05 | ||
13160.0 7.23784e-05 | ||
13190.0 6.48294e-05 | ||
13230.0 6.35979e-05 | ||
13260.0 7.54148e-05 | ||
13300.0 6.72707e-05 | ||
13330.0 6.41335e-05 | ||
13340.0 4.03223e-05 | ||
13360.0 2.09506e-05 | ||
13390.0 6.76998e-05 | ||
13430.0 5.13254e-05 | ||
13460.0 4.1107e-05 | ||
13490.0 1.80282e-05 | ||
13530.0 1.0643e-06 | ||
13550.0 1.47601e-08 | ||
13600.0 2.94853e-06 | ||
13630.0 3.30154e-07 | ||
13700.0 2.18978e-08 | ||
13730.0 2.70939e-06 | ||
13770.0 3.63108e-08 | ||
13830.0 0 | ||
13880.0 7.20461e-09 | ||
13920.0 2.37069e-07 | ||
13950.0 2.15054e-08 | ||
13960.0 6.08883e-07 | ||
13970.0 1.73228e-06 | ||
13980.0 8.88412e-06 | ||
14000.0 7.14286e-09 | ||
14010.0 7.14286e-09 | ||
14020.0 3.71612e-06 | ||
14040.0 7.40741e-07 | ||
14060.0 3.39972e-06 | ||
14070.0 2.84293e-08 | ||
14100.0 1.70213e-07 | ||
14120.0 3.75354e-07 | ||
14160.0 6.07345e-07 | ||
14210.0 4.92611e-08 | ||
14260.0 2.10379e-08 | ||
14420.0 2.77393e-08 | ||
14500.0 0 |
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Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,105 @@ | ||
# %ECSV 0.9 | ||
# --- | ||
# datatype: | ||
# - {name: wavelength, unit: Angstrom, datatype: float64} | ||
# - {name: response, datatype: float64} | ||
# meta: !!omap | ||
# - {band_name: Ks} | ||
# - {description: 'Instrument: 2MASS Cameras in Mt. Hopkins, AZ, and CTIO, Chile | ||
# | ||
# Determined by: Cohen, Wheaton & Megeath (2003), AJ, 126, 1990 with notes: | ||
# | ||
# "Table 1 - 2MASS Isophotal Bandpasses and Fluxes-for-0-magnitude from Cohen et al. (2003) | ||
# Band Lambda (micron) Bandwidth (micron) Fnu - 0 mag (Jy) Flambda - 0 mag (W cm-2 micron-1) | ||
# J 1.235 0.006 0.162 0.001 1594 27.8 3.129E-13 5.464E-15 | ||
# H 1.662 0.009 0.251 0.002 1024 20.0 1.133E-13 2.212E-15 | ||
# Ks 2.159 0.011 0.262 0.002 666.7 12.6 4.283E-14 8.053E-16 | ||
# | ||
# Figures 1, 2, and 3 present the 2MASS J, H and Ks relative spectral | ||
# response curves (RSRs), peak-normalized to unity. These curves are | ||
# derived by Cohen et al. (2003) and are photon-counting RSRs suitable | ||
# for integrating over stellar spectra when using or generating synthetic | ||
# photometry. These RSRs are consistent with the absolute calibration of | ||
# 2MASS given in Table 1 above." | ||
# | ||
# Notes: | ||
# I am not in a position to judge the quality of these curves, but | ||
# have no reason to doubt them. - Michael Blanton 2005-07-06'} | ||
# - {group_name: twomass} | ||
wavelength response | ||
18970.0 0 | ||
19150.0 0 | ||
19270.0 0 | ||
19340.0 1.03413e-08 | ||
19390.0 2.57865e-08 | ||
19480.0 2.77207e-07 | ||
19570.0 6.08074e-07 | ||
19620.0 1.00408e-06 | ||
19690.0 2.14322e-06 | ||
19760.0 4.41802e-06 | ||
19810.0 7.71328e-06 | ||
19890.0 1.24786e-05 | ||
19900.0 9.55779e-06 | ||
19980.0 1.17067e-05 | ||
20080.0 1.46713e-05 | ||
20140.0 1.97716e-05 | ||
20190.0 1.66716e-05 | ||
20280.0 3.06065e-05 | ||
20370.0 3.75552e-05 | ||
20450.0 3.64988e-05 | ||
20610.0 3.03299e-05 | ||
20720.0 3.50145e-05 | ||
20750.0 3.32289e-05 | ||
20820.0 3.78434e-05 | ||
20890.0 3.91623e-05 | ||
20990.0 3.91996e-05 | ||
21060.0 4.09924e-05 | ||
21130.0 4.15428e-05 | ||
21200.0 4.04561e-05 | ||
21240.0 4.22881e-05 | ||
21380.0 4.29794e-05 | ||
21450.0 4.32075e-05 | ||
21550.0 4.30023e-05 | ||
21690.0 4.15353e-05 | ||
21760.0 4.24081e-05 | ||
21850.0 3.85721e-05 | ||
21970.0 4.30542e-05 | ||
22080.0 4.44022e-05 | ||
22130.0 4.46408e-05 | ||
22180.0 4.44004e-05 | ||
22320.0 4.32213e-05 | ||
22370.0 4.38802e-05 | ||
22480.0 4.37455e-05 | ||
22560.0 4.26108e-05 | ||
22600.0 4.33274e-05 | ||
22630.0 4.41891e-05 | ||
22650.0 4.25254e-05 | ||
22700.0 4.32247e-05 | ||
22720.0 4.261e-05 | ||
22760.0 4.0022e-05 | ||
22770.0 4.31313e-05 | ||
22810.0 3.90004e-05 | ||
22840.0 3.90455e-05 | ||
22860.0 4.12249e-05 | ||
22910.0 3.66827e-05 | ||
22930.0 3.5072e-05 | ||
22950.0 3.08349e-05 | ||
22970.0 2.86281e-05 | ||
22990.0 2.43889e-05 | ||
23060.0 1.92411e-05 | ||
23110.0 1.50671e-05 | ||
23160.0 9.93955e-06 | ||
23200.0 7.00862e-06 | ||
23250.0 5.84946e-06 | ||
23280.0 3.95619e-06 | ||
23350.0 2.67238e-06 | ||
23390.0 1.84267e-06 | ||
23440.0 1.45051e-06 | ||
23460.0 1.3214e-06 | ||
23520.0 5.01701e-07 | ||
23610.0 2.88014e-07 | ||
23630.0 2.96234e-08 | ||
23700.0 1.26582e-07 | ||
23750.0 8.84211e-08 | ||
23840.0 1.67785e-08 | ||
23990.0 0 |
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