\begin{table}%T4
\caption{Oscillator strengths for some dipole-allowed
transitions, $f_{\rm L}$ and $f_{\rm V}$ are the present length and velocity
forms. OT represents other calculations. \label{tab4}}
%\centerline
 {
\begin{tabular}{c c c c c c c c}
\hline\hline
& & K VIII& & && Ti XI  &\\
I& J & $f_{\rm L}$ & $f_{\rm V}$& OT& $f_{\rm L}$ & $f_{\rm V}$& OT \\
\hline
\noalign{\smallskip}
$\rm 3s^2$($\rm ^1S_0$)&3s3p($\rm ^1P_1$)&1.1439&1.1602&$1.12^a,1.07^b$&.96513&.96619&
$.95^a,.918^b$ \\
  & & & &  $1.177^c,1.16^d, 1.1066^e$&& &$.9922^c,.98^d$ \\
3s3p($\rm ^1P_1$)&3s3d($\rm ^1D_2$)&1.0660&1.0904&$.986^d,
.9724^e$&.82693&.85534&$.78^d$  \\
$\rm 3p^2(^1S_0)$&3p3d($\rm ^1P_1$)&1.1538&1.2008& $1.10^d,
.9772^e$&.88631&.92450&$.85^d$  \\
$\rm 3p^2(^3P_1)$&3p3d($\rm ^3P_2$)&.35693&.37601&$.347^d, .3040^e$
&.35851&.37832&$.39^d$ \\
$\rm 3p^2(^3P_2)$&3p3d($\rm ^3D_3$)&.64512&.69546&$.62^d, .612^e$
&.46764&.50580&$.434^d$  \\
3s3p($\rm ^3P_0$)&$\rm 3p^2(^3P_1)$&.39671&.39061&$.40^d, .374^e$
&.33946&.32305&$.34^d$\\
3s3p($\rm ^3P_0$)&$\rm 3s3d(^3D_1)$&.52420&.54699&$.52^d, .5116^e$
&.40552&.41691&$.40^d$\\
3s3p($\rm ^3P_1$)&$\rm 3s3d(^3D_2)$&.39137&.41159&$.386^d, .3818^e$
&.30177&.31421&$.30^d$\\
3s3p($\rm ^3P_2$)&$\rm 3p^2(^3P_2)$&.29094&.28970&$.286^d, .2704^e$
&.23696&.23084&$.224^d$\\
3s3p($\rm ^3P_2$)&$\rm 3s3d(^3D_3)$&.43486&.46486&$.428^d, .4236^e$
&.33333&.35720&$.33^d$\\
\hline
\end{tabular}}
\smallskip
$^a$ Stanek et~al. (\cite{Stanek96}), $^b$ Safronova et~al.
(2000), $^c$ Huang \& Johnson (\cite{Huang85}), $^d$ Fawcett (\cite{Fawcett83}), $^e$
Bi\'emont et~al. (2002). 
\end{table}