Both WFPC2 and NICMOS are capable of imaging at wavelengths between ~8000Å and ~11,000Å. At longer wavelengths NICMOS must be used; at shorter wavelengths WFPC2, STIS, or ACS must be used. Table 1.3 compares the detective efficiency of WFPC2 and NICMOS in the wavelength region where both instruments overlap in capabilities. Count rates for a V=20 star of spectral class A0 are given for all filters at common wavelengths; the signal-to-noise (S/N) is also given for a 1 hour exposure of this same star. For bright continuum sources WFPC2 and NICMOS offer similar efficiency over the spectral range from 8800Å to 10,500Å; the choice of instrument will likely depend on other factors such as field size and details of the passband shape. However, for very faint sources, the lower read noise of WFPC2 (5e- for WFPC2 vs. 30e- for NICMOS) should prove advantageous.
Both instruments have polarimetry capability, but the WFPC2 polarizers are not viable above 8000Å; above this wavelength NICMOS must be used for polarimetry. We note that the ACS WFC is optimized for the far red and has polarimetric capability.
Instrument |
Filter |
Mean Wavelength (Å) |
Effective Width (Å) |
Count Rate (e- s-1) |
SNR in 1 hour1 |
---|---|---|---|---|---|
WFPC2 |
F785LP |
9366 |
2095 |
14 |
215 |
|
F791W |
8006 |
1304 |
30 |
314 |
|
F814W |
8269 |
1758 |
33 |
333 |
|
F850LP |
9703 |
1670 |
7.1 |
150 |
|
FQCH4N (Quad D) |
8929 |
64 |
0.47 |
34, 292 |
|
F953N |
9546 |
52 |
0.21 |
19, 15 2 |
|
F1042M |
10,443 |
611 |
0.20 |
18, 15 2 |
|
LRF3 |
8000 9000 9762 |
105 113 126 |
1.5 0.64 0.23 |
66 40 20 |
NICMOSe |
F090M4 |
8970 |
1885 |
17.4 |
89 |
|
F095N 4 |
9536 |
88 |
0.883 |
9.2 |
|
F097N 4 |
9715 |
94 |
1.19 |
12 |
|
F108N 4 |
10,816 |
94 |
1.17 |
9.9 |
|
F110W (Camera 1) |
11,022 |
5920 |
73 |
170 |
|
F110W (Camera 2) |
11,035 |
5915 |
83.7 |
290 |
|
F110W (Camera 3) |
11,035 |
5915 |
75.9 |
390 |
1WFPC2 SNR assuming two 1800s exposures for cosmic ray removal. NICMOS SNR for central pixel of PSF. 2Values given for WFC (0.10" pixels) and PC (0.046" pixels). 3LRF filter is continuously tunable from 3710Å to 9762Å. LRF field-of-view is 10"x10". 4These NICMOS filters are available only on Camera 1 which has 11"x11" field-of-view. 4e. The NICMOS ETC performs S/N calculations for the brightest pixel with the detector temperature at 77.1oK. |
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