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3. Observations

The survey consists of almost 8000 spectra which were taken between February and November 1984. The area observed covered tex2html_wrap_inline1816 and tex2html_wrap_inline2312. Spectra were obtained, both in longitude and latitude, every tex2html_wrap_inline1818 (0.85 beam-widths) for tex2html_wrap_inline1820, and every tex2html_wrap_inline1822 (1.7 beam-widths) for tex2html_wrap_inline1824.

Each spectrum was integrated for about 10 minutes, to yield an antenna temperature noise level of tex2html_wrap_inline1832 K (rms) for a 1.3 km s-1 velocity resolution (Table 2 (click here)). In order to subtract instrumental effects and the sky background the antenna was switched, every 15 seconds, between the target position (on) and an emission-free position (off) at elevations closer than tex2html_wrap_inline2326. The off positions were verified to have emission not greater than 0.04 K (Bitran 1987). Table 3 (click here) lists the emission-free positions.

Observations were carried out only under good weather conditions, i.e. when the zenith opacity of water vapor at 115 GHz was between 0.05 and 0.20. During the observations the spectra were examined visually and fitted with linear baselines only. If a spectrum showed evidence of baseline distortion it was discarded and the observation repeated.

  figure330
Figure 2: Spatial maps of CO line intensity tex2html_wrap_inline2328 integrated over the velocity range of -320 to 320 km s-1 displayed at three different contour levels. The contour intervals and the lowest contours have been set at 13, 32.5 and 65 K km s-1, corresponding to tex2html_wrap_inline2336 and tex2html_wrap_inline2338, in the top, middle and bottom maps, respectively



  figure341
Figure 5: Two longitude-velocity diagrams integrated below and above the galactic plane. The contour interval is 2 K, with the lowest contour at 2 K. The arrows point to two intense sources with unusually large velocity widths

Within tex2html_wrap_inline2340 of the galactic center the velocity span of the CO emission exceeded the full range of the spectrometer. This problem was circumvented by taking, for all positions within tex2html_wrap_inline2118, two spectra centered at velocities 306 km s-1 apart (Table 2 (click here)). These two spectra covered a combined range of 640 km s-1 with an overlap of 26 km s-1 (20 channels) allowing ample emission-free sections to set baselines, and enough overlap to check that the spectra matched properly (Fig. 1 (click here)). The emission level in the overlapping channels was checked to coincide in both spectra within the antenna temperature rms noise. Poor matchings were rejected and the corresponding positions re-observed. A sample of combined spectra along two adjacent longitude strips are shown in Fig. 1 (click here); the high signal-to-noise ratio and the flat baseline of these spectra are characteristics of the whole survey.

An important goal of this survey was to cover the full latitude extent of the galactic CO emission. We found most of the emission to be confined in tex2html_wrap_inline1820, therefore our latitude coverage (tex2html_wrap_inline2352) seems adequate. However, because HI emission is observed at higher latitudes in opposite galactic quadrants (at tex2html_wrap_inline2354 for tex2html_wrap_inline2356, and at tex2html_wrap_inline2358 for tex2html_wrap_inline2360), we conducted a search between tex2html_wrap_inline2362 and tex2html_wrap_inline2364 for tex2html_wrap_inline2356, and between tex2html_wrap_inline2368 and tex2html_wrap_inline2370 for tex2html_wrap_inline2360, detecting only local emission.


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