Astron. Astrophys. 328, L37-L39 (1997)
3. Observations and reductions
Crt has been observed in 6 out of 9 nights in
May 1997 at the National Astronomical Observatory, Rozhen, of the
Bulgarian Academy of Sciences, using the Coudé spectrograph at
the 2m RCC-telescope. The spectra were recorded with the ASTRO-550
system manufactured by Ista Ltd. (Berezin et al. 1991) with a virtual
phase CCD developed and produced by Electron
Corp., St. Petersburg, Russia) (see also Shcherbakov et al. 1995). The
camera was provided by the Helsinki University Observatory. The pixel
size is . The slit-width was set to 300
m, so that the FWHM of a typical comparison
line is about 2 pixels. The grating 632/ was
used, providing a dispersion of 0.01 nm per pixel. The total length of
the recorded spectra is thus about 6 nm. The observed wavelength
region is centered at 490 nm; in some nights additional spectra
centered at 505 nm were taken. The integration times were between 5
and 10 minutes. The signal-to-noise ratio of the spectra is typically
around 150. Due to the position of Crt,
observations were only possible very early in the night at very high
zenith-distances. The first of our spectra was taken too early, and is
heavily contaminated by a superposed solar spectrum.
During observations and reductions the 3A-software package (Ilyin
1993) has been used. The reductions contain the usual steps of bias
subtraction, flat-fielding, spectrum extraction and wavelength
calibration. The spectrum extraction was done by an algorithm similar
to the optimal extraction described by Horne (1986), getting rid of
the cosmics at the same time. The wavelength calibration is based on
typically 25 Fe and Ar lines, whose wavelengths are taken from the
catalogue by Hirata & Horaguchi (1995). The typical error of the
dispersion curve (being a polynomial of degree 1) is 0.26 pm,
corresponding to 0.16 km s-1 at 490 nm.
The external accuracy of the spectra and the reductions was checked
using spectra of the Sun (evening sky). One spectrum in each of the
two spectral regions was available. The positions of solar absorption
lines were measured by approximating them by Gaussians. The line
shifts then were computed by comparing with the wavelengths given by
Pierce & Breckinridge (1973). The mean shifts from many lines are:
km s-1 and
km s-1 for the spectra at 490 nm and 505 nm, respectively.
There are thus no significant systematics, and the main source of RV
errors for sharp lined spectra is the error of the dispersion
curve.
© European Southern Observatory (ESO) 1997
Online publication: March 26, 1998
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