The VLA observations and data reduction are discussed in FC89 and will
not be repeated here. The pertinent parameters are summarized in
Table 1.
The entire OH and HO maser database is presented in two tables and
one figure. Table 2 contains a list of reference positions for
each field observed. These are H
O maser positions, with the
exception of the eight instances where no H
O maser was detected and
the OH maser positions are used. Both B1950 and J2000 coordinates are
given, along with the kinematical distance and the synthesized beams
(major and minor axes and position angle of the restoring Gaussian).
The near and far distances are both listed unless there is no ambiguity.
If the ambiguity has not been resolved but one distance is preferred,
the other is enclosed in parentheses. For the 23 GHz continuum
detections and the sense of circular polarization used for the OH
observations, Table 1 of FC89 should be consulted.
The source names used are the same as in FC89. These are derived from
the galactic coordinates of the OH maser reference positions, and may
differ slightly from the galactic coordinates of the HO masers
listed in Table 2. There is one additional field in
Table 2 which was not listed in FC89. 8.68-0.37 is an isolated
OH maser approximately 1 arcmin from the OH/H
O maser association
8.67-0.36. This specific OH maser site has been referred to in several
publications (e.g. Caswell 1998) and has therefore been given a
separate listing here. There are three other fields which contain maser
sites with large separations (348.70-1.04, 12.22-0.12 and 23.01-0.41),
but these are listed as single entries for consistency with FC89.
While a position for 19.61-0.13 is given in Table 2, this weak,
isolated OH maser is not included in Table 3 or in Fig. 1
since only one spectral channel was positioned and there is no
associated HO maser.
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Spectra and positions for the OH and HO masers in each field are
plotted in Fig.1. There are a total of 74 spot maps in the complete
figure, which is only available in electronic form. An example for the
field 351.42+0.64 (NGC6334N) is printed here as Fig. 1. The source
name is given at the top left of the sky plot, and the OH and H
O
beam sizes are shown schematically to the right (OH beam cross-hashed).
Note that the beams are not to scale, but have the correct position
angle and aspect ratio. Table 2 should be consulted for the
size of the beams in arc seconds. Linear size scales are given to the
right of each sky plot, with the near and far distances (if ambiguous)
printed at the top of each scale. The symbols in the sky plot are
crosses (
) for OH and circles (
) for H
O. The corresponding grayed symbols represent the mean
position of the maser spots for that species (note that the grayed
crosses become gray squares). The grayed symbols do not necessarily
correspond to an actual maser position. The star symbol, if present,
represents the position of the continuum peak detected at 23 GHz.
Below the sky plots are the OH and HO maser spectra measured at the
VLA. The two maser species are plotted on the same velocity scale, and
the scale for each field spans a fixed range of 80 km s-1 for ease of
comparison. Each spectrum has one filled (darker) symbol denoting the
median velocity of each species. For fields in which only one
species was detected, only one spectrum is shown.
Below the spectra are listed the following values derived from the spot maps. If no continuum source or only one maser species was detected some items are not displayed. Linear sizes in mpc are given for both near and far distances.
Several minor modifications have been made to the original FC89
database. First, the assumed distance has been revised from 2.0 to 5.7 kpc
for 9.62+0.20 (Hofner et al. 1994). Second, deep imaging
of the continuum emission at 9 GHz has been obtained for fields between
353 and 25
galactic longitude (Forster & Caswell, in preparation).
The new observations show that three of the 23 GHz continuum detections
listed in FC89 (359.14+0.03, 359.62-0.25, and 12.91-0.26) are spurious.
These have therefore been removed from the FC89 database. In addition,
new observations of OH and H
O masers and Hii regions toward some
of the fields in FC89 have provided independent measurements of the
absolute positions. These are discussed in the next section. Finally,
a misprint in FC89 for the reference position of the OH maser 11.90-0.14
has been corrected.
Copyright The European Southern Observatory (ESO)