\begin{table}%t2
\caption{Optimized decomposition of the sub-damped profile shown in 
Fig.~\ref{fg:dla}. The listed numbers correspond to a straight continuum, 
for a curved continuum the errors increase. The origin of the radial 
velocity scale corresponds to the redshift $z=1.15080$.
Note that the non-damped absorption does provide only little information.
The line parameters are listed for completeness only.}\label{tb:dla}
%\centering
\small
\begin{tabular}{@{}lccl@{}}
\hline
\hline
Transition\rule[0pt]{0pt}{10pt}
& $\phantom{-}v_{\rm r}$
& $b$
& $\log N$
\\
\rule[-5pt]{0pt}{0pt}
& $\phantom{-}$(km~s\ensuremath{^{-1}})
& (km~s\ensuremath{^{-1}})
& (cm\ensuremath{^{-2}})
\\
\hline
\ion{H}{i} 1216\rule{0pt}{10pt}
& $-3.19 \pm 11.14$
& $75.17 \pm 5.84$
& $19.89 \pm 0.03$
\\  
\ion{H}{i} 1216
& $-236.14$
& $82.74 \pm 7.23$
& $16.84 \pm 0.92$
\\
\ion{H}{i} 1216
& $-533.51$
& $82.74 \pm 7.23$
& $14.98 \pm 0.13$
\\
\hline
\end{tabular}
\end{table}