\begin{table}%t1
\caption{Map parameters for {sources of} the complete 
S5~polar cap sample at~15.4~GHz.}\label{table:results-mapping}
%\centerline
{
  \begin{tabular}{rcrrrccrrrc}
\hline  \hline
& \mcthc{----------- Epoch 1999.57 -----------} &&
& \mcthc{----------- Epoch 2000.46 -----------}  
\\
& \mctwc{Beam {\it FWHM}$^{a}$} & & & 
& \mctwc{Beam {\it FWHM}$^{a}$} & & 
\\
\mconc{\bf Source}  
& \mconc{Size} & {PA} & {$S_{\rm peak}$} & {$S_{\rm tot}$$^{b}$} 
& {\scriptsize rms level$^{c}$}
& \mconc{Size} & {PA} & {$S_{\rm peak}$} & {$S_{\rm tot}$$^{b}$}
& {\scriptsize rms level$^{c}$}
\\
& \mconc{[mas]} & & {\scriptsize [mJy/beam]} & {\scriptsize [mJy]} 
& {\scriptsize [mJy/beam]}
& \mconc{[mas]} & & {\scriptsize [mJy/beam]} & {\scriptsize [mJy]}
& {\scriptsize [mJy/beam]}
\\ \hline
{\bf \object{QSO~0016+731}} & 0.619 $\;\times\;$ 0.396 & 6\fdg4	 &  487 &  647 & 0.5 & 0.643 $\;\times\;$ 0.392 &   6\fdg9  & 694 & 817 & 0.6 \\
{\bf \object{QSO~0153+744}} & 0.860 $\;\times\;$ 0.352 & --6\fdg9  &  163 &  316 & 1.0 & 0.853 $\;\times\;$ 0.345 & --4\fdg9  & 169 & 312 & 0.7 \\
{\bf \object{QSO~0212+735}} & 0.899 $\;\times\;$ 0.371 & --3\fdg3	 & 1025	& 2529 & 0.5 & 0.869 $\;\times\;$ 0.366 & --3\fdg4  &1032 & 2507 & 0.6 \\
{\bf \object{BL~0454+844}}  & 0.425 $\;\times\;$ 0.362 & 57\fdg5	 &   59	&  120 & 0.4 & 0.393 $\;\times\;$ 0.370 &  70\fdg9   & 71 & 131 & 0.4 \\
{\bf \object{QSO~0615+820}} & 0.451 $\;\times\;$ 0.401 & 22\fdg6	 &  129	&  434 & 0.7 & 0.475 $\;\times\;$ 0.392 &  16\fdg4  & 148 & 410 & 0.7 \\
{\bf \object{BL~0716+714}}  & 0.853 $\;\times\;$ 0.344 & --4\fdg9	 & 1024	& 1107 & 0.8 & 0.845 $\;\times\;$ 0.326 & --2\fdg7  & 968 & 1051 & 0.7 \\
{\bf \object{QSO~0836+710}} & 0.885 $\;\times\;$ 0.345 & --15\fdg9 & 1259	& 1766 & 0.8 & 0.898 $\;\times\;$ 0.336 & --12\fdg5 & 1147& 1728 & 0.6 \\
{\bf \object{QSO~1039+811}} & 0.621 $\;\times\;$ 0.390 & --18\fdg3 &  737	&  926 & 0.6 & 0.546 $\;\times\;$ 0.365 & --11\fdg7 & 584 & 826 & 0.9 \\
{\bf \object{QSO~1150+812}} & 0.626 $\;\times\;$ 0.310 &--39\fdg0	 &  316 &  946 & 0.8 & 0.659 $\;\times\;$ 0.345 & --37\fdg2 & 358 & 907 & 0.6 \\
{\bf \object{BL~1749+701}}  & 1.044 $\;\times\;$ 0.359 &--7\fdg3	 &  229	&  382 & 0.7 & 1.268 $\;\times\;$ 0.405 & --16\fdg8 & 261 &  405 & 0.9 \\
{\bf \object{QSO~1803+784}}  & 0.571 $\;\times\;$ 0.374 &--3\fdg0	 & 1965 & 2878 & 0.8 & 0.533 $\;\times\;$ 0.426 & 15\fdg3   & 1524& 2313 & 0.9 \\
{\bf \object{QSO~1928+738}} & 1.090 $\;\times\;$ 0.376 & 15\fdg9	 & 1492 & 3006 & 1.0 & 1.371 $\;\times\;$ 0.394 & 8\fdg1	 & 1214& 2889 & 0.8 \\
{\bf \object{BL~2007+777}}  & 0.487 $\;\times\;$ 0.429 & --30\fdg1 &  384	&  825 & 0.4 & 0.488 $\;\times\;$ 0.422 &--49\fdg1  & 680 & 1258 & 0.5 \\ \hline
\end{tabular}}
\medskip
$^{a}$ The restoring beam is an elliptical Gaussian
with full-width-half-maximum ({\it FWHM}) axes $a$~$\times$ $b$.
For each source, the position angle~(PA) stands for the direction of the
major axis measured north through east. \\
$^{b}$ Total flux density recovered in the hybrid mapping process. \\
$^{c}$ Contours in the maps of the figures shown  in Sects.~\ref{subsec:0016} to~\ref{subsec:2007}
are the tabulated rms values times $(-3,3,3\sqrt{3},9,\cdots)$.
\end{table}