| Space Telescope Imaging Spectrograph Instrument Handbook for Cycle 14 | |||||
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F28X50OIII-CCD
Description
The
F28X50OIIImode is useful for narrow-band imaging of O III 5007 Å. The narrow bandpass and high spatial resolution provides some advantages over WFPC2 with the F502N filter, although the spatial resolution is not as high as that of ACS/HRC with its F502N filter.Recommended Uses
Recommended for deep high-resolution O III imaging.
Special Considerations
This filter has a significant red leak longward of 1 micron. Depending on the source spectrum, the contribution from redleak may swamp the contribution from line emission.
Figure 14.12: Throughput for F28x50OIII.
Table 14.6: Throughput and Sensitivity for F28X50OIII
Figure 14.13: Point Source S/N vs. V+ABfor the F28X50OIII filter.Top curves are for low sky; bottom curves are for average sky. Curves are labeled by required exposure time (sec).
Figure 14.14: Extended Source S/N vs. V+ABfor the F28X50OIII for gain=1. Top curves are for a source area of 0.2 arcsec2; bottom curves are for 1 arcsec2. Average sky assumed. Curves are labeled by required exposure time (sec).
Table 14.7: Radial Profile for F28X50OIII
Figure 14.15: Point Source PSF for F28X50OIII, 7."5 square (pixel 493,542, log scaled, B-V=-0.34)
Figure 14.16: Point Source Encircled Energy for F28X50OIII
Figure 14.17: Point Source Intensity vs. Radius for F28X50OIII
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