\begin{table}%t1
\caption{\label{table}Results of  modelling  of continuum and broad  \HI~absorption profiles along the jet axis (see Sect.~3.3).}
%\centering
\par
\begin{tabular}{r r c c c}
\hline\hline\noalign{\smallskip}
$r$ & $F_{\rm C}$  & $F_{\rm L}$  & $F_{\rm L}$$F_{\rm C}^{-1}$  & $\tau_0$  \\
 (mas)  & (mJy) & (mJy)   &    &  \\
\hline
--60 & 4.73 & 0.23 & $0.05 \pm 0.12$ & $0.080 \pm 0.210$\\
--45 & 3.62 & 4.06 & $1.12 \pm 0.15$ & ${>}3.110$\\
--30 & 0.02 & 0.00 & 0.00 & --\\
--15 & 22.78 & 4.24 & $0.19 \pm 0.02$ & $0.320 \pm 0.040$\\
0 & 139.16 & 1.57 & $0.01 \pm 0.004$ & $0.016 \pm 0.006$\\
15 & 0.00 & 0.00 & -- & --\\
30 & 20.98 & 0.00 & $0.00 \pm 0.03$ & $0 \pm 0.0478$\\
\hline
\end{tabular}
\tablefoot {Column~1 give the distance from the core of the fitted pixel, negative offsets correspond to positions along the counter-jet, positive to positions on the jet side. Columns~2 to~4 give respectively the  fitted continuum flux density, \HI~absorbed flux density averaged over fitted frequency range and the line to continuum ratio. Column~5 gives the modelled opacity at line~centre.}
\end{table}