\begin{table}%t8
\caption{The relative line strengths of the Fe II multiplet $a^{6}$D--$z^{6}$D.\label{tab8}}
%\centerline
{\begin{tabular}{cccr} 
\hline\hline
Transition & $\lambda_{\rm vac}$(lab) (\AA) & {\it gA}$^{a}$ & $I^{b}$ \\  \hline
9/2--9/2   &  2600.17  &  2.39  &    0$^{c}$  \\
9/2--7/2   &  2586.65  &  0.37  &    0$^{c}$  \\
7/2--9/2   &  2626.45  &  0.75  & 1.23        \\
7/2--7/2   &  2612.65  &  1.00  & 1.00        \\
7/2--5/2   &  2599.15  &  0.32  & 0.39        \\
5/2--7/2   &  2632.11  &  0.87  &   bl        \\
5/2--5/2   &  2618.40  &  0.30  & 0.92        \\
5/2--3/2   &  2607.87  &  0.45  & 0.61        \\
3/2--5/2   &  2631.83  &  0.70  &   bl        \\
3/2--3/2   &  2621.19  &  0.02  & 0.72        \\
3/2--1/2   &  2614.61  &  0.37  & 0.47        \\
1/2--3/2   &  2629.08  &  0.43  & 0.53        \\
1/2--1/2   &  2622.45  &  0.12  & 0.52        \\ \hline
\end{tabular} }
\par
\smallskip 
 $^{a}$ The gA values from Schnabel et~al. (2004) are scaled in such a way that gA for the 
$a^{6}$D$_{7/2}$--$z^{6}$D$_{7/2}$ transition is equal to 1.00. \\
 $^{b}$ The observed intensity relative to $I$($a^{6}$D$_{7/2}$--$z^{6}$D$_{7/2}$) = 1.00. \\
 $^{c}$ Both transitions to the ground level $a^{6}$D$_{9/2}$ are observed in \mbox{absorption}.
\end{table}