All Figures

$\begin{figure} \par\includegraphics[angle=-90,width=15cm,clip]{0384fig1.eps} \end{figure}$ Figure 1: Collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^3P_1$ - $\rm 3s^23p^4$ $\rm ^3P_2$ transition in Cl II as a function of electron energy (Ryd) in the thresholds energy region.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=15cm,clip]{0384fig2.eps} \end{figure}$ Figure 2: Collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^3P_1$ - $\rm 3s^23p^4$ $\rm ^1D_2$ transition in Cl II as a function of electron energy (Ryd) in the thresholds energy region.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=16cm,clip]{0384fig3.eps} \end{figure}$ Figure 3: Collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^1D_2$ - $\rm 3s^23p^4$ $\rm ^1S_0$ transition in Cl II as a function of electron energy (Ryd) in the thresholds energy region.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{0384fig4.eps} \end{figure}$ Figure 4: Collision strength for the allowed $\rm 3s^23p^4$ $\rm ^1D_2$ - $\rm 3s^23p^3(^2D^{\circ })4s$ $\rm ^1D^{\circ }_2$ (solid curve), $\rm 3s^23p^4$ $\rm ^3P_1$ - $\rm 3s^23p^3(^4S^{\circ })4s$ $\rm ^3S^{\circ }_1$ (long-dashed curve) and $\rm 3s^23p^4$ $\rm ^1D_2$ - $\rm 3s^23p^3(^2D^{\circ })3d$ $\rm ^1P^{\circ }_1$ (short-dashed curve) transitions in Cl II as a function of electron energy (Ryd) above the highest excitation threshold.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{0384fig5.eps} \end{figure}$ Figure 5: Effective collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^3P_0$ - $\rm 3s^23p^4$ $\rm ^3P_1$ transition in Cl II as a function of log T (K). Solid curve, present results; dashed-curve, Wilson & Bell.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{0384fig6.eps} \end{figure}$ Figure 6: Effective collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^3P_1$ - $\rm 3s^23p^4$ $\rm ^1D_2$ transition in Cl II as a function of log T (K). Solid curve, present results; dashed-curve, Wilson & Bell.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{0384fig7.eps} \end{figure}$ Figure 7: Effective collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^3P_1$ - $\rm 3s^23p^4$ $\rm ^1S_0$ transition in Cl II as a function of log T (K). Solid curve, present results; dashed-curve, Wilson & Bell.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{0384fig8.eps} \end{figure}$ Figure 8: Effective collision strength for the forbidden $\rm 3s^23p^4$ $\rm ^1D_2$ - $\rm 3s^23p^4$ $\rm ^1S_0$ transition in Cl II as a function of log T (K). Solid curve, present results; dashed-curve, Wilson & Bell.
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In the text