The true polarization parameters in the sky reference frame for 154 sources are presented in Table 4. Columns (1) and (2) give the right ascension - declination designations and an alternative catalogue number. Columns (3) and (4) give their position in right ascension and declination (1950) while Cols. (5) and (6) provide their galactic position in degrees. Column (8) through (13) display the flux and its error, the degree of polarization and its error, and the position angle of the plane of polarization and its errors, respectively. Where the error in m exceeds the value of m itself, no position angle is quoted.
Figure 1a shows the distribution of the linear
polarization values for all sources measured. The results were
generated using the polarization
data in Table 4, but corrected for noise bias
mentioned in the preceeding section. The noise bias is greatest when
the polarized flux signal-to-noise
. Since all sources, except
for one, have flux densities greater than 100 mJy, this effect is only
seen when
. Considering the bin size used in the
figure, very little change should occur between the corrected and
uncorrected m6.3 values. In fact, when we apply the
Wardle-Kronberg estimator (Wardle & Kronberg 1974;
Simmons & Stewart 1985), the only difference in the
binned data is that the noise corrections displaced one value from the
bin to the
bin in Fig. 1.
For those sources with known redshift, we compare in Figs. 1b and c the distribution of linear polarization values for sources above and below z=0.5.
A full analysis of the Faraday rotation properties of these sources awaits the completion of measurments at other wavelengths and will be presented elsewhere.
E.L.H.Z. and P.P.K. thank the Natural Sciences and Engineering Research Council of Canada for support of this work. We thank Gabi Breuer and W. Fußhöller for their assistance with the manuscript.
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