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2. Observations and maps

In order to cover the 3 600 square degrees area contained between tex2html_wrap_inline1250, four different data sets were used. The strip delimited by tex2html_wrap_inline1252 and tex2html_wrap_inline1254 was sampled by the surveys of Weaver & Williams (1973) from tex2html_wrap_inline1256 to tex2html_wrap_inline1258, and Strong et al. (1982) from tex2html_wrap_inline1260 to tex2html_wrap_inline1262. The region outside this band was surveyed by Heiles & Habing \ (1974) and Colomb et al. (1977, 1980). In Fig. 1 (click here), the observed points in each survey are plotted. Regions of overlap among the different surveys were used to control the quality of the match. Since several regions appear quite under-sampled, unpredictable errors can be produced after the processing and combination of the data. Therefore, we avoid the analysis of small scale structure. In what follows, a brief description of the different surveys is given:

  figure238
Figure 1: Distribution of the observed points in each survey. Open triangles correspond to the survey of Heiles & Habing (1974); open circles, to Colomb et al. (1977, 1980); filled circles, to Strong et al. (1982); and filled triangles, to Weaver & Williams (1973)

a) Weaver & Williams (1973): this atlas covers a regular grid in tex2html_wrap_inline1264, with an interval of tex2html_wrap_inline1266 in longitude and tex2html_wrap_inline1268 in latitude. Observations were performed over an area of tex2html_wrap_inline1270, tex2html_wrap_inline1272, using the 26 m telescope of Hat Creek, Berkeley, with an angular resolution of tex2html_wrap_inline1274. The noise level was 0.38 K in antenna temperature. The relation between antenna and brightness temperature is tex2html_wrap_inline1276 The profiles consist of 200 velocity channels spaced in tex2html_wrap_inline1278 \ (except for the extreme channels, not used in the present study, for which tex2html_wrap_inline1280 is different), and the reference velocity, which in general varies for each profile, is referred to channel 122.

b) Heiles & Habing (1974): observations were also made with the 26 m telescope of Hat Creek, Berkeley, in the region observable from the local latitude and for tex2html_wrap_inline1282. In this case, the sampling was irregular in tex2html_wrap_inline1284, with tex2html_wrap_inline1286 and tex2html_wrap_inline1288. The southern limit of the sample was tex2html_wrap_inline1290. The noise level was in general less than 0.4 K. The data are given in antenna temperature, with tex2html_wrap_inline1292. The profiles, with 100 velocity channels, have a velocity interval of tex2html_wrap_inline1294 , except for the first eight and last five channels, for which tex2html_wrap_inline1296 . The reference velocity, 0 in almost all the profiles, is refered to channel 52.

c) Colomb et al. (1977, 1980): observations were taken with the 30 m radiotelescope of the IAR, with a resolution of tex2html_wrap_inline1298 at 1420 MHz. This survey has been performed with the purpose of being combined with the survey of Heiles and Habing, giving a complete coverage of the sky at tex2html_wrap_inline1300. The data were obtained by scanning in Right Ascention for fixed declination, with tex2html_wrap_inline1302 between scans. The velocity resolution is 2 . The velocity range is about 80 , and the first channel velocity varies from one profile to the other. The data are given in antenna temperature, with tex2html_wrap_inline1304.

d) Strong et al. (1982): observations were taken with the 64 m radiotelescope at Parkes, with an angular resolution of tex2html_wrap_inline1306 at 1420 MHz. The spectral resolution was 0.824 , and the number of velocity channels, 512. This survey covers the area tex2html_wrap_inline1308, tex2html_wrap_inline1310, with a regular sampling in galactic coordinates with tex2html_wrap_inline1312 and tex2html_wrap_inline1314. The reference velocity, at the central channel, is 0 , except for the strip delimited by tex2html_wrap_inline1316, tex2html_wrap_inline1318, where this velocity is +50 . The noise level is 1 K. Due to the rather low signal-to-noise ratio, a Hanning smoothing was applied, which lowered the velocity resolution of the profiles to 1.648 and the rms noise level to 0.6 K. The data were corrected for a systematic shift of 2.6 in velocity (Dubner et al. \ 1992). No beam smoothing was applied.

All data were converted into brightness temperature and fitted into one single field, within the velocity range tex2html_wrap_inline1320 , in 2 velocity intervals, with a uniform grid in galactic coordinates. Each grid point profile was calculated as the weighted mean among the four nearest profiles (one per quadrant). In the zone of overlap between the Strong et al. and the Weaver & Williams surveys, only profiles from the former were used. The final product was a set of spectral data placed each tex2html_wrap_inline1322 in l and tex2html_wrap_inline1326 in b. The images were processed using the AIPS software. The rms noise level of each channel is better than 1 K.


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