Astron. Astrophys. 346, 45-57 (1999)
2. Observations
2.1. Interferometric 12CO observations
Interferometric 12CO
observations were obtained at the Owens Valley Radio Observatory
(OVRO) millimeter array. The six 10.4 m telescopes are equipped with
SIS receivers providing system temperatures of typically
K (single sideband). Details of the
observations are given in Table 2. With natural weighting, we
obtained a roughly circular beam of size
(PA 46o and sensitivity
to extended structure up to 17". The quasar 2345-167 was observed as a
phase and amplitude calibrator every
minutes. Passband calibration was
done using stronger sources, usually 0528+134 or 3C 454.4. These
sources, calibrated against the planets Neptune and Uranus, were also
taken for flux calibration. The tracks were calibrated using software
developed for the OVRO array. After calibration, the data were
inspected for quality, and low-coherence data points were edited out
on a baseline-to-baseline basis.
![[TABLE]](img14.gif)
Table 2.
Summary of the interferometric observations.
Notes:
a) The array configurations at OVRO are labelled C (compact), L (low resolution) and H (high resolution)
For a beam size of , a brightness
temperature ( ) of 1 K corresponds to
0.304 Jy beam-1 at a wavelength of 2.6 mm. The spectral
resolution of our data is 4 MHz or 10.04 km s -1, and the
total velocity range covered by the autocorrelator is 1120 km s
-1, centered on =
1200 km s -1.
Imaging was done using the NRAO AIPS package. To cover the long bar
of UGC 2855 fully, we obtained a 3-field mosaic with a spacing of
between the pointing centers. The
fields were CLEANed individually and combined linearly, correcting for
the attenuation of the primary beam, using the AIPS task LTESS.
To analyse the innermost structure (see Sect. 4.1), the beam size
could be reduced to (PA
78o) applying robust weighting (Briggs 1995), while a beam
size of (PA -19o) was
reached when only the longer baseline data from the high resolution
track were used. This (naturally weighted, since the signal-to-noise
in the robustly weighted maps is too low) map includes baselines from
230 m to 35 m length, which means that structures larger than
cannot be imaged. The increased
resolution also goes along with a loss in sensitivity: The rms noise
per channel increases from 0.11 K
(34 mJy beam-1) in the naturally weighted map to 0.43 K
(52 mJy beam-1) in the robustly weighted and 1.34 K
(62 mJy beam-1) in the high-resolution-only maps.
The interferometric 12CO observations of UGC 2866 are
summed up in Table 2. The naturally-weighted map of UGC 2866 has
a beam size of (PA -68o)
and an rms noise of 0.20 K (38 mJy beam-1). The velocity
resolution, velocity range and central velocity of these observations
were the same as those of UGC 2855.
2.2. Interferometric 13CO observations
Data in the 13CO
transition of the same three fields in UGC 2855 (see Table 2)
that were mapped in 12CO were taken at OVRO in June 1998
under excellent weather conditions, using the same spectrometer
configuration as for 12CO. The calibration and mapping
procedure was identical to the 12CO measurements. The
(naturally weighted) synthesised beam has a size of
(PA
), and the sensitivity reached is
0.09 K
(23 mJy beam-1).
2.3. Single-dish observations of UGC 2855
Single dish 12CO and
13CO data of UGC 2855
were obtained with the 20 m telescope at Onsala Space Observatory in
December 1997 and January 1998. We observed 7 spectra along the bar in
12CO, spaced by 15" along the bar, and 5 positions in
13CO (see Fig. 3). The central position
( almost exactly coincided with the
interferometric CO emission peak. The typical system temperature was
500 K - 600 K for 12CO and 200 K - 300 K for
13CO. The beam size is ,
and the spectra have been smoothed to a velocity resolution of
km s -1. The Onsala
spectra do not fully sample the entire area of the OVRO interferometer
map and have pointing uncertainties of
, preventing us from combining the
single-dish data with the interferometry data into a single map.
2.4. H
An H image of UGC 2855 and UGC 2866
was taken using HoLiCam (Reif et al. 1995) at the 1.06 m telescope at
Hoher List Observatory in October 1997. The conditions were not
photometric, and the image provides relative information on fluxes
only. However, no other deep H imaging
of these galaxies is available at this time. The image was processed
using the IRAF package.
© European Southern Observatory (ESO) 1999
Online publication: May 6, 1999
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