$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig1.eps} } \end{figure}$ Figure 1: Collision strength as a function of incident electron energy in rydbergs for the 2s2p² ⁴P_1/2-2s2p² ²D_5/2 fine-structure forbidden transition.
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In the text

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig2.eps} } \end{figure}$ Figure 2: Present effective collision strength as a function of log (T) where T is the electron temperature in kelvin for the 2s2p² ⁴P_1/2-2s2p² ²D_5/2 fine-structure forbidden transition (solid line) compared with the results of Blum & Pradhan (1992) (dashed line).
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In the text

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig3.eps} } \end{figure}$ Figure 3: Collision strength as a function of incident electron energy in rydbergs for the 2s2p² ²D_3/2-2s²3p ²P ${\rm ^o}_{3/2}$ fine-structure allowed transition.
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In the text

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig4.eps} } \end{figure}$ Figure 4: The effective collision strength as a function of log (T) where T is the electron temperature in kelvin for the 2s2p² ²D_3/2-2s²3p ²P $^{\rm o}_{3/2}$ fine-structure allowed transition (solid line) compared with the results of Blum & Pradhan (1992) (dashed line).
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In the text

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig5.eps} } \end{figure}$ Figure 5: Comparison of the current collision strength (solid line) with experimental data for the 2s²2p ²P $^{\rm o}$ -2s2p² ²D excitation: Williams et al. (1998) crossed beams (filled circles); Smith et al. (1996) merged beams (open squares).
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In the text

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig1.eps} } \end{figure}$	Figure 1: Collision strength as a function of incident electron energy in rydbergs for the 2s2p² ⁴P_1/2-2s2p² ²D_5/2 fine-structure forbidden transition.
Open with DEXTER

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig2.eps} } \end{figure}$	Figure 2: Present effective collision strength as a function of log (T) where T is the electron temperature in kelvin for the 2s2p² ⁴P_1/2-2s2p² ²D_5/2 fine-structure forbidden transition (solid line) compared with the results of Blum & Pradhan (1992) (dashed line).
Open with DEXTER

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig3.eps} } \end{figure}$	Figure 3: Collision strength as a function of incident electron energy in rydbergs for the 2s2p² ²D_3/2-2s²3p ²P ${\rm ^o}_{3/2}$ fine-structure allowed transition.
Open with DEXTER

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig4.eps} } \end{figure}$	Figure 4: The effective collision strength as a function of log (T) where T is the electron temperature in kelvin for the 2s2p² ²D_3/2-2s²3p ²P $^{\rm o}_{3/2}$ fine-structure allowed transition (solid line) compared with the results of Blum & Pradhan (1992) (dashed line).
Open with DEXTER

$\begin{figure} \par {\includegraphics[width=8.8cm,clip]{1855fig5.eps} } \end{figure}$	Figure 5: Comparison of the current collision strength (solid line) with experimental data for the 2s²2p ²P $^{\rm o}$ -2s2p² ²D excitation: Williams et al. (1998) crossed beams (filled circles); Smith et al. (1996) merged beams (open squares).
Open with DEXTER