Up: VLA observations of a
The observations were performed
using the VLA in
B-configuration
at a frequency centred on 4860.1 MHz, on four
occasions: 1994 July 8, 1994 July 30, 1995
October 9 and 1995 December 10. Data
were taken in two contiguous
bands of 50 MHz bandwidth centred
at 4835 MHz and 4885 MHz.
Exposure times were 2 minutes, resulting in a
theoretical rms noise level of 0.10 mJy/beam;
the median noise level of the
maps is in fact about 0.1 mJy/beam (estimated from
the rms in the bottom 20 pix2 of each map).
Phase calibration was performed typically once every
10-15 sources using point-source calibrators from
the VLA Calibrator List
(Perley 1982)
during the 1995 observations, although only sporadic
phase calibration is available for the 1994
observations. Flux densities were bootstrapped to the
source 3C 48, using the value of 5.4 Jy at 4850 MHz from
Baars et al. (1979).
After calibration in AIPS, the data on each
source in turn were mapped using the
Caltech Difmap package
(Shepherd et al. 1995),
typically involving one pass of phase
selfcalibration and one of amplitude
self-calibration between passes through the CLEAN
algorithm, using windows to build up
flux in successively fainter parts of the source.
A few sources (nearly all of them
bright point sources) had residual offset corrections
applied in addition. The final
dataset was then read back into AIPS and the CLEAN
algorithm was applied using the task
IMAGR with the ROBUST parameter set to zero, giving
a weighting scheme intermediate
between natural and uniform weighting. In a few cases
the Difmap CLEANed map was used
as the final map. The combination of the two algorithms
allowed easy interactive
investigations of the data combined with deep and thorough
CLEANing.
For each component
of each object, the peak and extended fluxes have been
measured by hand using the AIPS
task TVSTAT. This procedure gives an indication of the
flux, although it may not be
totally reliable in cases where components are not well
resolved from each other or
when components are large and extended, and hence partially
resolved out by the
interferometer. Where a core was seen on the map, this was
measured separately;
otherwise a value is typically quoted for each lobe of a
double source. 19 objects
overlap with the sample observed in Paper I at 1.4GHz.
Basic observational parameters
are given in Table 1,
namely the date of the observation,
details of the point-source
response in the map, and comments about the data analysis.
In Table 2 we present the
flux and position measurements for the individual components,
and indicate by an asterisk those cases in which the core is
likely to be detected (although lacking spectral indices for
each component we cannot identify the cores definitely).
Figure 1 shows the maps of the sources. The noise level in each
observation can be deduced from Fig. 1, in which the lowest
contour is 2.8 times the rms noise level. In some cases only
point sources are visible. In these cases, however, there is
sometimes an indication of further resolved structure which
the observations do not have the spatial frequency coverage to
map properly.
A few, mostly small, sources were also mapped using
the MERLIN interferometer at L-band (
1.4 GHz). The dates
and details of these observations are given in Table 3, and the
resulting maps in Fig. 2.
Acknowledgements
The Very Large Array is operated by Associated Universities for
Research in
Astronomy Inc. under agreement with the National
Science Foundation. MERLIN is operated as a National Facility
by the University of Manch ester on behalf of the UK Particle
Physics and Astronomy Research Council.
Table 1:
Objects observed, together with the major and minor axis (in arcseconds)
and position angle (in degrees) of the restoring beam. Epochs are numbered as
follows: 1=1994 July 8; 2=1994 July 30; 3=1995 October 9; 4=1995 December
10
![\begin{table}
\includegraphics [clip]{tab1a.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img11.gif) |
Table 1:
continued
![\begin{table}
\includegraphics [clip]{tab1b.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img12.gif) |
Table 1:
continued
![\begin{table}
\includegraphics [clip]{tab1c.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img13.gif) |
Table 2:
Positions of sources observed with the VLA, together
with flux (mJy)es derived from the maps (see text).
Both peak and integrated fluxes are given. Probable cores are indicated
by an asterisk
![\begin{table}
\includegraphics [clip]{tab2a.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img14.gif) |
Table 2:
continued
![\begin{table}
\includegraphics [clip]{tab2b.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img15.gif) |
Table 2:
continued
![\begin{table}
\includegraphics [clip]{tab2c.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img16.gif) |
Table 2:
continued
![\begin{table}
\includegraphics [clip]{tab2d.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img17.gif) |
Table 2:
continued
![\begin{table}
\includegraphics [clip]{tab2e.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img18.gif) |
Table 2:
continued
![\begin{table}
\includegraphics [clip]{tab2f.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img19.gif) |
Table 3:
Log of the MERLIN observations
![\begin{table}
\includegraphics [clip]{table3.eps}
\end{table}](/articles/aas/full/1999/03/ds1513/img20.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1a.eps}\end{figure}](/articles/aas/full/1999/03/ds1513/Timg21.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1b.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg22.gif) |
Figure 1:
VLA maps of the sources observed. The bottom
contour is indicated on the map (in mJy) in each case, and is always
2.8 times the rms noise level. The contour levels are (-1, 1, 1.4,
2.03, 3.05, 4.7, 7.6, 12.5, 21.2, 37, 67, 123, 235 , 457, 915, 1880, 4000)
times the bottom contour |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1c.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg23.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1d.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg24.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1e.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg25.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1f.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg26.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1g.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg27.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1h.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg28.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1i.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg29.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1j.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg30.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1k.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg31.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1l.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg32.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1m.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg33.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1n.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg34.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1o.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg35.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1p.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg36.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1q.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg37.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1r.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg38.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1s.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg39.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1t.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg40.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1u.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg41.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1v.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg42.gif) |
Figure 1:
continued |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1w.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg43.gif) |
![\begin{figure}
\includegraphics [height=20cm,clip]{fig1x.eps}
\end{figure}](/articles/aas/full/1999/03/ds1513/Timg44.gif) |
Figure 1:
continued |
 |
Figure 2:
MERLIN maps of six small
sources observed in Paper I. Contours are given at
(-1, 1, 2, 4, 8, 16, 32...)
where
f = 1 mJy/beam (4C+00.15),
0.5 mJy/beam (4C+03.14), 0.7 mJy/beam
(4C+00.31), 0.5 mJy/beam (4C-02.63),
0.3 mJy/ beam (4C-03.65),
1.5 mJy/beam (4C+00.80) |
Up: VLA observations of a
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