next previous
Up: A radio continuum

2. The five Parkes surveys

Table 1 (click here) lists the characteristics of the five SMC surveys used in this study of discrete sources. We consider the region of tex2html_wrap_inline1132 6tex2html_wrap_inline1134  tex2html_wrap_inline1136 7tex2html_wrap_inline1138 centred on Right Ascension (B1950) tex2html_wrap_inline1140 and Declination (B1950) -73tex2html_wrap_inline1144 00tex2html_wrap1236 00tex2html_wrap1238 which cover tex2html_wrap_inline1150 square degrees between RA tex2html_wrap_inline1152 to tex2html_wrap_inline1154 and Dec tex2html_wrap_inline1156tex2html_wrap_inline1158 40tex2html_wrap1240 to -76tex2html_wrap_inline1164 20tex2html_wrap1242 .

  table219
Table 1: Parameters of the five radio surveys of the SMC

The four primary surveys of the SMC at 1.42, 2.45, 4.75 and 8.55 GHz were made between 1988 and 1991 using the Parkes 64-m telescope fitted with the Australia Telescope National Facility's prototype receiver package (Haynes et al. 1986, 1991). Observations at these four frequencies were made by scanning the telescope across the SMC in right ascension and declination at driving rates in the range 1tex2html_wrap_inline1200 to 4tex2html_wrap_inline1202 tex2html_wrap_inline1204. At each observing frequency we used 1-s integration for each datum point and made 2.3 measurements across each beam size in the scanning direction. The beam size ranged from 13.8tex2html_wrap1244 to 2.7tex2html_wrap1246 depending on the observing frequency (Table 1 (click here)). The resulting images exhibited some scanning ``noise" (caused by variations in the absorbing emission characteristics of the Earth's atmosphere) which depended on the scanning direction. These scanning effects have been efficiently removed by the so-called ``basket-weaving" technique developed at the MPIfR (Sieber et al. 1979).

Calibration was undertaken by frequently observing sources with known integrated flux density and position, and by mapping them in the same manner as for the MCs (Haynes et al. 1991; Paper IV). The main source for flux-density calibration was Hydra A. The adopted integrated flux density scale is that determined by Baars et al. (1977). As secondary calibrators (mainly used for pointing calibration) we chose the sources 3C 348, 3C 353, B0332-403, B0843-336, B1819-67, B1934-638 and B2356-61.

For the 1.42-GHz survey, the primary calibrator was Virgo A (for which an integrated flux density of 213 Jy was assumed), while the secondary calibrators were Hydra A, 3C 138, B1414+11, B1814-63 and B1819-67 (Haynes et al. 1986).

Our fifth study at 4.85 GHz used a public-release FITS image of the SMC obtained from the PMN survey. The PMN Southern Survey was made with the Parkes telescope in 1992 (Griffith et al. 1991, 1994; Griffith & Wright 1993; Wright et al. 1994). Radio images between declination range -88tex2html_wrap_inline1226 tex2html_wrap_inline1228tex2html_wrap_inline1230 at 4.85 GHz are available in FITS format with a 4.9tex2html_wrap1248 initial resolution and an rms. noise between 5 and 13 mJy tex2html_wrap_inline1234. We have taken these PMN survey FITS images which cover the region of the SMC and used the NOD2 source-fitting package to determine source positions and flux densities.


next previous
Up: A radio continuum

Copyright by the European Southern Observatory (ESO)
web@ed-phys.fr