The redshifts of the objects were determined from low resolution
spectra obtained
using the KPNO Cryogenic Camera and the Lick Cassegrain CCD
Spectrograph. With
the Cryocam we used the 810 lines mm grating, GG420 order
sorting filter, and 2.5"
slit, corresponding to a wavelength resolution of about 30A and a
pixel separation of 0.84"
and 10 Åin the spatial and wavelength directions respectively. The
Lick spectrograph was
used in the UV mode with a 2.0" slit, corresponding to a wavelength
resolution of 8 Åper
pixel and a pixel separation of 0.66" in the spatial and wavelength
directions respectively.
With both instruments the observing procedure was to center a nearby
star in the slit of
the spectrograph and then offset the telescope to the position of the
optical identification.
The data were reduced with IRAF. The CCD data were bias subtracted,
and flat fielded
with a spectral flats made by dividing a polynomial fit to the tungsten
lamp source. The
wavelength scale was fit with a 5th order polynomial for the Cryocam
and a 3rd order
for the Lick UV Spectrograph. Redshifts were determined for sources
with two or more
emission lines. Follow up intermediate resolution long slit
spectroscopy is presented in
Chambers et al. 1996b (Paper III).