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The 4-m Ritchey-Chretien Focus Spectrograph is the primary spectroscopic
work-horse for optical spectroscopy at Kitt Peak. There are a dozen
diffraction gratings available, which provide resolutions from 300 to
5000. It uses the ``UV Fast Camera" to focus
the spectrum onto a CCD detector. The CCD currently in use with the
RC Spectrograph is a Tektronix 2048
detector with excellent cosmetics.
The total system throughput (telescope + spectrograph + CCD) is
11-14% under typical seeing conditions with a nominal slit width (18% peak
under excellent seeing conditions).
The spectrograph is normally used in long-slit mode (slit length=5.2
)
for either two-dimensional spectroscopy of extended sources
or for spectroscopy of point sources with excellent sky subtraction.
In this (normal) mode, a slit-viewing TV (field of view 2.5')
provides the means for
acquisition. However, the spectrograph can also be used with multi-slit
masks. The instrument rotator at the 4-m
allows remote control of the position angle of the slit
on the sky, although such rotations need to be done with the
telescope within 30
of zenith. Thus the spectrograph can be rotated to the parallactic
angle (to keep all of the light down the slit), or, if you need to
use a particular position angle, you can use the atmospheric dispersion
corrector (``Risley prisms"); see Sec. 4.4.1.
The focus of the RC Spectrograph begins to degrade on the red side (large pixel numbers) past pixel 1500, with poor resolution and substantial vignetting past pixel 1700. A similar focus degradation occurs on the blue side between pixels 0 and 200.
A list of the available gratings with the resulting wavelength coverage, dispersion, and resolution, is given below. We give the wavelength coverage both for 1500 pixels, to which people doing demanding work may want to restrict themselves, and for 1700 pixels, which may be suitable for some qualitative applications. The laboratory measurements of the grating efficiences are shown in Fig. 2 and Fig. 3.
Notes: (a) Based on 2.5 pixels FHWM
corresponding to 300

m slit (2 arcsec). Better resolution can
be achieved with smaller slit widths. (b) Spectral coverage limited
by overlapping orders. (c) Spectral coverage limited by grating
efficiency and atmospheric cut-off.
Figure 2: The efficiencies of the various RC gratings
are shown here (continued on the next figure).
Figure 3: The efficiencies of the various RC gratings
are shown here (continued from the previous figure).
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