Low dispersion spectra of 117 galaxies were obtained in several observing runs since 1995 using the imaging spectrographs BFOSC and LFOSC attached to the Cassini 1.5 m telescope (Loi) at Loiano (Italy) and the 2.1 m telescope (Can) of the Guillermo Haro Observatory at Cananea (Mexico), respectively.
The observations at Loiano were performed using a 2.0 or 2.5 arcsec slit, depending on the seeing conditions, oriented E-W. The exposure time ranged between 20 and 90 min according to the brightness of the target object. Observations at Cananea were carried out with a 3.1 arcsec fixed slit, oriented N-S. Every galaxy spectrum was preceded and followed by an exposure of a HeAr lamp (Loiano) or XeNe lamp (Cananea) to secure the wavelength calibration.
Data reduction was performed in the IRAF-PROS environment.
After bias subtraction, when 3 or more frames of the same target
were obtained, these were combined (after spatial alignment)
using a median filter to help cosmic rays removal.
Otherwise the cosmic rays were removed under visual inspection.
The wavelength calibration was checked on known sky lines. These were
found within Å from their nominal value, providing an
estimate of the systematic uncertainty on the derived velocities of
.
After subtraction of the sky background, one-dimensional spectra were
extracted from the frames.
These spectra were analyzed with either of two methods:
1) individual line measurement: all spectra taken at Cananea and those
obtained at Loiano prior to 1996 were inspected and emission/absorption
lines were identified. Emission lines include H, N[II] and S[II].
Absorption lines include the Mg[I], CaFe and Na.
The galaxy redshift was obtained from these individual measurements.
If more than one line was identified, the galaxy redshift was derived as
the weighted mean of the individual measurements, with weights
proportional to the line intensities.
2) Cross correlation technique: spectra obtained at Loiano after 1996
were analyzed using the cross-correlation technique of
Tonry & Davis (1979).
This method is based on a "comparison" between the spectrum of a galaxy whose
redshift is to be determined, and a fiducial spectral template
of a galaxy (or star) of appropriate spectral type to contain the wanted
absorption/emission lines.
The basic assumption behind this method is that the spectrum of a
galaxy is well approximated by the spectrum of its stars, modified
by the effects of the stellar motions inside the galaxy
and by the systemic redshift.
For this purpose high signal-to-noise spectra
were taken of two template galaxies: M105 (absorption lines)
and NGC 1330 (emission lines), whose redshifts are 866 and 1039 respectively.
The observed redshifts () were first transformed to Heliocentric
(
), then corrected for the motion of our galaxy
relative to the Cosmic Microwave Background (
) according to
Kogut et al. (1993).
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