\begin{table}%T2
%\centering
\par
\caption{Comparison of our theoretical results for Stark broadening of 
Ge~I lines with experimental 
results. 
With $W_{\rm m}$  are denoted experimental full widths at half maximum in 
[\AA] and with $W_{\rm e}$ and $W_{\rm GeII}$ our theoretical values for Stark 
widths due to electron- and 
Ge~II-impacts, respectively. Accuracy is denoted as in Konjevi\'c et al. (\cite{Konjevi84}) and 
Konjevi\'c \& Wiese (\cite{Konjevi90}), C means that error bars are within $\pm$50\% and 
D$^+$ 
that they are  larger than $\pm$50\%. Under Ref., 1 is for Musiol et al. (\cite{Musiol88}) 
and 2. for Jones \& Miller (\cite{Jones74}).}\label{tab2}
\par
\begin{tabular}{|c|c|c|c|c|c|c|c|c|}
\hline\hline
Transition & $\lambda $(\AA)& $T$(K)&$N_{\rm e}$ & $W_{\rm m}$ & $W_{\rm e}$ & $W_{\rm Ge II}$ & Acc. & Ref. \\
& & & $10^{17}$~cm$^{-3}$ &(\AA) &(\AA) &(\AA) & &  \\
\hline
%\hline
4p$^2$ $^3$P--5s$^3$P$^0$ &2754.59 &12~450 &0.57 &0.0509 &0.0502 &0.00644 &C     &1 \\
                           &2709.62 &12~450 &0.57 &0.0434 &0.0490 &0.00628 &C     &1 \\
                           &2651.57 &12~450 &0.57 &0.0358 &0.0466 &0.00596 &C     &1 \\
                           &2651.17 &12~450 &0.57 &0.0427 &0.0517 &0.00662 &C     &1 \\
                           &2592.53 &12~450 &0.57 &0.0452 &0.0494 &0.00633 &C     &1 \\
\hline
4p$^2$ $^1$S--5s$^3$P$^0$ &4685.83 &11~000 &1    &0.35   &0.248  &0.0339  &C     &2 \\
\hline
4p$^2$ $^1$D--5s$^3$P$^0$ &3124.82 &12~450 &0.57 &0.0628 &0.0715 &0.00928 &C     &1 \\
\hline
4p$^2$ $^1$D--5s$^1$P$^0$ &3039.07 &12~450 &0.57 &0.0622 &0.0721 &0.00924 &C     &1 \\
\hline
4p$^2$ $^1$S--5s$^1$P$^0$ &4226.56 &11~000 &1    &3.18   &0.239  &0.0318  &C     &2 \\
                           &        &12~450 &0.57 &0.0815 &0.139  &0.0185  &D$^+$ &1 \\
\hline
\end{tabular}
\end{table}