$\begin{figure} \par\includegraphics[width=8.8cm,clip]{4152fig1.eps} \end{figure}$ Figure 1: A partial level diagram of Cr II showing the levels investigated in this work. Left hand side shows the sextet levels and right hand the quartets. Since the LS-coupling in Cr II is not pure, intercombination lines are seen between the quartet and sextet systems.
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In the text

$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig2.eps}}} } \end{figure}$ Figure 2: Comparision between log gf-values from our work and the work of Bergeson & Lawler (1993). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Bergeson}$ is plotted as a function of line strength.
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In the text

$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig3.eps}}} } \end{figure}$ Figure 3: Comparision between log gf-values from our work and the work of Gonzalez et al. (1994). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Gonzales}$ is plotted as a function of line strength.
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In the text

$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig4.eps}}} } \end{figure}$ Figure 4: Comparison between log(gf) values from our work and the work of Spreger et al. (1994). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Spreger}$ is plotted as a function of line strength.
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In the text

$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig5.eps}}} } \end{figure}$ Figure 5: Comparision between log gf-values from our work and the work of Musielok & Wujec (1979). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Musielok}$ is plotted as a function of line strength.
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In the text

$\begin{figure} { \rotatebox{-90}{ \resizebox{!}{8.8cm}{\includegraphics{4152fig6.eps}}} } \end{figure}$ Figure 6: Comparision between log gf-values from our work and Kurucz (1988). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Kurucz}$ is plotted as a function of line strength.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{4152fig1.eps} \end{figure}$	Figure 1: A partial level diagram of Cr II showing the levels investigated in this work. Left hand side shows the sextet levels and right hand the quartets. Since the LS-coupling in Cr II is not pure, intercombination lines are seen between the quartet and sextet systems.
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$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig2.eps}}} } \end{figure}$	Figure 2: Comparision between log gf-values from our work and the work of Bergeson & Lawler (1993). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Bergeson}$ is plotted as a function of line strength.
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$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig3.eps}}} } \end{figure}$	Figure 3: Comparision between log gf-values from our work and the work of Gonzalez et al. (1994). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Gonzales}$ is plotted as a function of line strength.
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$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig4.eps}}} } \end{figure}$	Figure 4: Comparison between log(gf) values from our work and the work of Spreger et al. (1994). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Spreger}$ is plotted as a function of line strength.
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$\begin{figure} { \rotatebox{-90}{\resizebox{!}{8.8cm}{\includegraphics{4152fig5.eps}}} } \end{figure}$	Figure 5: Comparision between log gf-values from our work and the work of Musielok & Wujec (1979). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Musielok}$ is plotted as a function of line strength.
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$\begin{figure} { \rotatebox{-90}{ \resizebox{!}{8.8cm}{\includegraphics{4152fig6.eps}}} } \end{figure}$	Figure 6: Comparision between log gf-values from our work and Kurucz (1988). $\Delta$ log( $gf)= \log(gf$ ) $_{\rm This~Work} -\log(gf$ ) $_{\rm Kurucz}$ is plotted as a function of line strength.
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