Astronomical Spectroscopy - Physics - University of Cincinnati
Astronomical Spectroscopy - Physics - University of Cincinnati
Astronomical Spectroscopy - Physics - University of Cincinnati
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– 45 –<br />
be obtained for each grating setting and filter combination you use during the night,<br />
the same as with optical data. Furthermore, they should be obtained with exposure<br />
levels that push to the linearity limits in order to maximize the signal-to-noise ratio.<br />
This linearity limit can be as low as 10,000 e − for some IR detectors. However, unlike<br />
the case for the optical, one must also obtain an equivalent set (in terms <strong>of</strong> exposure<br />
time and number) <strong>of</strong> dome flats with the dome illumination turned <strong>of</strong>f, as the dome<br />
flat itself is radiating in the NIR. One can demonstrate the necessity for this by a<br />
simple experiment: subtract an image obtained with the lamps turned <strong>of</strong>f from an<br />
image with the lamps turned on, and see how many counts there really are over the<br />
entire wavelength range. One may be surprised how many counts were removed from<br />
the original exposure, particularly in the longer wavelength K band. But it is this<br />
subtracted dome flat that will be used to flatten the data frames, so there needs to<br />
be a lot <strong>of</strong> counts in it in order not to reduce the signal-to-noise! For the K band,<br />
where there is high background counts and because the dynamic range <strong>of</strong> the detector<br />
is small, one may need 20 or more flat-on, flat-<strong>of</strong>f pairs to get sufficient real signal.<br />
• Quartz flats will be taken during the night, but daytime exposures will test the<br />
exposure levels and reveal any structural differences between it and the dome and<br />
twilight flats. Of course, dark frames with matching integration times will be needed.<br />
• Comparison lamps should be taken throughout the night, but obtaining a few during<br />
the day may also prove to be useful. Be sure to get dark frames to match the integration<br />
time.<br />
During the night, one will take:<br />
• Telluric standard stars are (nearly) featureless stars that will be used to derive the<br />
spectrum <strong>of</strong> the telluric absorption bands for removal from the program data. These<br />
are not spectrophotometric stars. They must be chosen to lie at similar (within 0.1)<br />
airmasses as the target stars for the reasons explained above, and observed within an<br />
hour or two <strong>of</strong> the target (more <strong>of</strong>ten for observations beyond 3µm).<br />
• Quartz Lamps may be useful or not, depending upon the specific instrument.<br />
• Comparison lamp exposures are a good idea. In the infrared, one can almost always<br />
use the night sky emission lines as the wavelength reference source. But separate<br />
comparison lamp exposures may prove useful if there turns out not to be enough<br />
counts in the sky lines, or if some regions are too void <strong>of</strong> sky lines, such as the long-K<br />
region. It is also a good idea to take these if you are moving the grating <strong>of</strong>ten, the<br />
program integration times are short, or if the dispersion is high.