The leftmost column contains the command name. The following two columns
show the filter combination's central wavelength and FWHM. Next are the
two filter wheel positions (inner and outer). The sixth column gives an
estimate of the background rate in electrons/sec (using 6 electrons/DN).
This of course can vary from night to night, and position in the sky. The
seventh column gives an estimate of the sensitivity, in the form of a "zero-point"
magnitude. This is 2.5 times the log (base 10) of the number of electrons/sec
expected from a zeroth magnitude star. Note that standard star measurements
exist only for standard passbands; all other estimates (shown in italics)
are approximate. Also note that atmospheric conditions will cause the apparent
sensitivity to vary from night to night. The icons in the last column link
to plots of the individual filter passbands.
Macro |
Wavelength |
FWI |
FWO |
Background |
Sensitivity |
Plot? |
CMD |
Central |
FWHM |
Pos |
Pos |
electrons/sec |
|
|
Broad-Band Filters |
|
z |
1.03225 |
0.1565 |
2 |
19 |
|
|
|
j |
1.251 |
0.292 |
3 |
10 |
2000 |
28.13 |
|
jh |
1.30 |
0.60 |
1 |
10 |
|
|
|
h |
1.6575 |
0.333 |
4 |
10 |
6400 |
27.80 |
|
hk |
1.967 |
1.13 |
9 |
19 |
|
|
|
kp |
2.1235 |
0.337 |
6 |
19 |
3800 |
26.92 |
|
ks |
2.155 |
0.33 |
7 |
19 |
3600 |
26.78 |
|
k |
2.2135 |
0.427 |
8 |
19 |
7200 |
27.16 |
|
kw |
2.249 |
0.594 |
10 |
19 |
30,000 |
27.50 |
|
ch4 |
2.269 |
0.155 |
5 |
10 |
|
|
|
ls |
2.9785 |
1.023 |
12 |
19 |
3,200,000* |
26.62 |
|
kl |
3.1475 |
2.003 |
14 |
19 |
|
|
|
lw |
3.492 |
1.490 |
15 |
19 |
45,000,000 |
26.94 |
|
lp |
3.831 |
0.620 |
13 |
19 |
9,700,000* |
26.24 |
|
lm |
3.945 |
2.002 |
17 |
19 |
|
|
|
m |
4.718 |
0.628 |
16 |
19 |
95,000,000 |
24.87 |
|
mw |
5.022 |
1.356 |
18 |
19 |
|
|
|
Thermal Blocking Filters |
|
uv22i |
1.45 |
2.5 |
11 |
19 |
|
|
|
uv22o |
1.45 |
2.5 |
19 |
10 |
|
|
|
Narrow-Band Filters |
|
hei |
1.0829 |
0.0136 |
19 |
0 |
49 |
24.70 |
|
pgamma |
1.0930 |
0.0104 |
11 |
1 |
47 |
24.62 |
|
oii |
1.23605 |
0.0105 |
19 |
2 |
86 |
24.31 |
|
pbeta |
1.2823 |
0.0146 |
11 |
3 |
350 |
24.72 |
|
feii |
1.6471 |
0.0176 |
11 |
4 |
330 |
24.12 |
|
h210 |
2.12495 |
0.0235 |
11 |
11 |
150 |
22.98 |
|
brgamma |
2.1647 |
0.0224 |
11 |
12 |
200 |
23.21 |
|
h221 |
2.24855 |
0.0239 |
11 |
13 |
138 |
22.95 |
|
kcont |
2.25965 |
0.0531 |
19 |
15 |
570 |
24.43 |
|
co20 |
2.2973 |
0.0274 |
19 |
14 |
240 |
23.41 |
|
pahcs |
3.0825 |
0.1007 |
19 |
16 |
285,000 |
24.25 |
|
pah |
3.3100 |
0.063 |
19 |
17 |
540,000 |
23.53 |
|
pahl |
3.4128 |
0.0734 |
19 |
18 |
490,000 |
23.92 |
|
bralphacont |
3.9923 |
0.0483 |
19 |
5 |
930,000 |
23.51 |
|
bralpha |
4.0455 |
0.0524 |
19 |
6 |
1,320,000 |
23.40 |
|
* Empirical fits of the background rate as a function of airmass, AM:
- Background rate in Ls = (1.8 * AM + 1.4) x 10^6 electrons/sec
- Background rate in L' = (2.8 * AM + 6.9) x 10^6 electrons/sec
Remember in these formulae that AM is always greater than or equal to
1!
These formulae can be interpreted as a sky background rate, which depends
on AM, and a telescope+instrument background rate, which is independent
of AM.
Last Update: 1/29/98
Name: Bob Goodrich
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