Filters

Filter FWHM (Å) CWL (Å) Telescope Instrument Plot Data Comments
BrG_G1122 308.00 21660.00 Gemini South GSAOI BrG_G1122 BrG_G1122
CaT_G0333 1525.00 8600.00 Gemini South GMOS-S CaT_G0333 CaT_G0333
CH4long_G1110 1057.00 16900.00 Gemini South GSAOI CH4long_G1110 CH4long_G1110
CH4short_G1109 919.00 15800.00 Gemini South GSAOI CH4short_G1109 CH4short_G1109
CO2360_G1124 788.00 23600.00 Gemini South GSAOI CO2360_G1124 CO2360_G1124
EO_466 440.00 4670.00 Gemini South ZORRO EO_466 EO_466 not convolved with dichroic
EO_562 437.00 5622.00 Gemini South ZORRO EO_562 EO_562 not convolved with dichroic
EO_716 515.00 7159.00 Gemini South ZORRO EO_716 EO_716 not convolved with dichroic
EO_832 403.00 8320.00 Gemini South ZORRO EO_832 EO_832 not convolved with dichroic
FeII_G1118 258.00 16440.00 Gemini South GSAOI FeII_G1118 FeII_G1118
g_G0325 1547.00 4750.00 Gemini South GMOS-S g_G0325 g_G0325
GG455_G0329 0.00 0.00 Gemini South GMOS-S GG455_G0329 GG455_G0329
H 2902.00 16310.00 Gemini South FLAMINGOS2 H H
H_G1103 2855.00 16350.00 Gemini South GSAOI H_G1103 H_G1103
H-alpha 32.00 6565.00 Gemini South ZORRO H-alpha H-alpha not convolved with dichroic
H2(1-0)_G1121 293.00 21220.00 Gemini South GSAOI H2(1-0)_G1121 H2(1-0)_G1121
H2(2-1)_G1123 314.00 22480.00 Gemini South GSAOI H2(2-1)_G1123 H2(2-1)_G1123
H20_G1119 734.00 20000.00 Gemini South GSAOI H20_G1119 H20_G1119
H6073 Gemini South Phoenix H6073 Start (cm-1 μm): 6017=1.662 - Stop (cm-1 μm): 6129=1.632 - Echelle order 34
H6420 Gemini South Phoenix H6420 Start (cm-1 μm): 6377=1.568 - Stop (cm-1 μm): 6464=1.547 - Echelle order 36
Ha_G0336 71.00 6560.00 Gemini South GMOS-S Ha_G0336 Ha_G0336
HaC_G0337 70.00 6620.00 Gemini South GMOS-S HaC_G0337 HaC_G0337
Hcont_G1108 234.00 15700.00 Gemini South GSAOI Hcont_G1108 Hcont_G1108
HeI-2p2s_G1120 284.00 20580.00 Gemini South GSAOI HeI-2p2s_G1120 HeI-2p2s_G1120
HeI1083_G1115 163.00 10830.00 Gemini South GSAOI HeI1083_G1115 HeI1083_G1115
HeII_G0340 74.00 4680.00 Gemini South GMOS-S HeII_G0340 HeII_G0340
HeIIC_G0341 75.00 4780.00 Gemini South GMOS-S HeIIC_G0341 HeIIC_G0341
HK 12541.00 18710.00 Gemini South FLAMINGOS2 HK HK
i_G0327 1440.00 7800.00 Gemini South GMOS-S i_G0327 i_G0327
J 1593.00 12550.00 Gemini South FLAMINGOS2 J J
J_G1102 1584.00 12500.00 Gemini South GSAOI J_G1102 J_G1102
J_LOW 1447.00 11220.00 Gemini South FLAMINGOS2 J_LOW J_LOW
J7799 Gemini South Phoenix J7799 Start (cm-1 μm): 7750=1.290 - Stop (cm-1 μm): 7865=1.271 - Echelle order 44
J8265 Gemini South Phoenix J8265 Start (cm-1 μm): 8243=1.213 - Stop (cm-1 μm): 8360=1.196 - Echelle order 47. Currently not installed in Phoenix.
J9232 Gemini South Phoenix J9232 Start (cm-1 μm): 9183=1.089 - Stop (cm-1 μm): 9286=1.077 - Echelle order 52
J9440 Gemini South Phoenix J9440 Start (cm-1 μm): 9396=1.064 - Stop (cm-1 μm): 9497=1.053 - Echelle order 53
J9671 Gemini South Phoenix J9671 Start (cm-1 μm): 9652=1.036 - Stop (cm-1 μm): 9709=1.030 - Echelle order 55. Currently not installed in Phoenix.
Jcont_G1107 199.00 12070.00 Gemini South GSAOI Jcont_G1107 Jcont_G1107
JH 9030.00 13900.00 Gemini South FLAMINGOS2 JH JH
K_BLUE 2421.00 20600.00 Gemini South FLAMINGOS2 K_BLUE K_BLUE
K_G1106 3240.00 22000.00 Gemini South GSAOI K_G1106 K_G1106
K_LONG 5837.00 22000.00 Gemini South FLAMINGOS2 K_LONG K_LONG
K_RED 2650.00 23100.00 Gemini South FLAMINGOS2 K_RED K_RED
K_SHORT 3299.00 21570.00 Gemini South FLAMINGOS2 K_SHORT K_SHORT
K4132 Gemini South Phoenix K4132 Start (cm-1 μm): 4077=2.452 - Stop (cm-1 μm): 4156=2.406 - Echelle order 23. Currently not installed in Phoenix.
K4220 Gemini South Phoenix K4220 Start (cm-1 μm): 4188=2.392 - Stop (cm-1 μm): 4263=2.348 - Echelle order 24
K4308 Gemini South Phoenix K4308 Start (cm-1 μm): 4258=2.349 - Stop (cm-1 μm): 4355=2.296 - Echelle order 24
K4396 Gemini South Phoenix K4396 Start (cm-1 μm): 4355=2.296 - Stop (cm-1 μm): 4446=2.249 - Echelle order 25
K4484 Gemini South Phoenix K4484 Start (cm-1 μm): 4429=2.250 - Stop (cm-1 μm): 4525=2.210 - Echelle order 25
K4578 Gemini South Phoenix K4578 Start (cm-1 μm): 4525=2.210 - Stop (cm-1 μm): 4630=2.160 - Echelle order 26
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