\begin{table}%T4
\caption{Fe$^{+22}$: comparing the present wavelengths $\lambda$(R) and 
weighted oscillator strengths $gf$(R) from AUTOSTRUCTURE with those of 
 Bathia \& Mason (\citeyear{bhatia_mason:81},
 \citeyear{bhatia_mason:86}), 
$\lambda$(BM) and $gf$(BM);  
 \cite{bhatia_etal:86}, $\lambda$(BFS); 
\cite{fawcett:84}, $\lambda$(F) and $gf$(F); 
\cite{sampson_etal:84}; $gf$(SGC);  
\cite{murakami_kato:96}, $\lambda$(MK); 
\cite{guo-xin_ong:98a}, $\lambda$(GO) and $gf$(GO); 
Fawcett's laboratory measurements (\citealt{fawcett_etal:79}), 
$\lambda$(Exp). 
Wavelengths are in \AA.}
\label{oscillator}
%\centering
\par
\begin{tabular}{lllllllllllll}
\hline\hline\noalign{\smallskip}
$\lambda$(R) 
& $\lambda$(BM)
&  $\lambda$(BFS)
& $\lambda$(F)
& $\lambda$(MK)
& $\lambda$(GO)
& $\lambda$(Exp)
&$gf$(R)
&$gf$(BM)
&$gf$(F)
&$gf$(SGC)
&$gf$(GO)
 & Transition \\
\hline
%&&&&&&&&&&&&\\[-2mm]
%\par
 11.0063&
 11.00 & 11.018 
&11.017&11.006 
&11.018 & 11.022 & 2.525$^{-1}$ 
&2.4$^{-1}$ &2.7$^{-1}$&2.4$^{-1}$ & 2.679$^{-1}$ &$1-13$ \\
\par
10.9697  & 
 10.97 &10.978
&10.979& 10.966 
&10.979 & 10.983 &4.092$^{-1}$ 
&4.06$^{-1}$ &4.5$^{-1}$&4.7$^{-1}$  & 4.110$^{-1}$ & $1-15$ \\
%\par
%&&&&&&&&&&&&\\[-2mm]
%\par
10.6645 &  
& &  & & &
&1.297$^{-2}$ & && &1.290 $^{-2}$ &$1-22$ \\
\par
10.4960& 
& & & & &
&2.342$^{-2}$ & && & 2.198 $^{-2}$& $1-25$ \\
%\par
%&&&&&&&&&&&&\\[-2mm]
%\par
10.3448&  
&& & & &
&5.025$^{-3}$ && & & 5.810 $^{-3}$ &$1-36$ \\
\par
10.2272&  
&&  & & 
&
&2.001$^{-4}$&&&& 2.336 $^{-4}$&  $1-42$ \\
\par
10.1520&  
&& & &
&  
&1.745$^{-2}$&&& &1.932 $^{-2}$& $1-46$ \\
%\par
%&&&&&&&&&&&&\\[-2mm]
%\par
8.3072&  & & &8.3059 & 8.316 &
&2.673$^{-2}$ && & & &$1-50$ \\
\par
8.2956&  & & &8.2934 &8.303 &
&1.339$^{-1}$& && & &$1-52$ \\
%\par
%&&&&&&&&&&&&\\[-2mm]
%\par
8.0753&  
& & & &
&
&3.112$^{-4}$ & && & & $1-62$ \\
\par
7.9931&  
&& & &
& 
&2.987$^{-4}$&&&& &$1-75$ \\                         
%\par
%&&&&&&&&&&&&\\[-2mm]
%\par
7.9994&  & & & & & & 2.347$^{-3}$ & & && & $1-70$ \\
%\par
%&&&&&&&&&&&\\[-2mm]
%\par
7.9258&
&& & &
&  
&6.297$^{-5}$&& && &$1-87$ \\
\par
7.9102&  
&& & &
&  
&4.574$^{-3}$&& && &$1-97$ \\
\hline
\end{tabular}
\end{table}