$\begin{figure} \par\subfigure[\bf {}]{\includegraphics[angle=-90,width=7.7cm,cli... ...ure[]{\includegraphics[angle=-90,width=7.7cm,clip]{3057fig1b.ps} }\end{figure}$ Figure 1: Partial collision strengths for the (3s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
Open with DEXTER

In the text

$\begin{figure} \par\subfigure[]{\includegraphics[angle=-90,width=8cm,clip]{3057f... ...igure[]{\includegraphics[angle=-90,width=8cm,clip]{3057fig2b.ps} }\end{figure}$ Figure 2: Partial collision strengths for the 3s²3p⁵ ²P $_{3/2}^\circ {-}3$ s3p⁶ ²S_1/2 (1-3) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
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In the text

$\begin{figure} \par\subfigure[]{\includegraphics[angle=-90,width=8cm,clip]{3057f... ...igure[]{\includegraphics[angle=-90,width=8cm,clip]{3057fig3b.ps} }\end{figure}$ Figure 3: Partial collision strengths for the 3s3p⁶ ²S _1/2-3s²3p⁴(¹S)3d ²D_5/2 (3-26) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8cm,clip]{3057fig4.ps} \end{figure}$ Figure 4: Partial sums of collision strengths for the 3s²3p⁵ ²P $_{3/2}^\circ {-}3$ s3p⁶ ²S_1/2 (1-3) transition of Fe X, at three energies of 18 Ryd (circles), 27 Ryd (triangles), and 45 Ryd (stars).
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In the text

$\begin{figure} \par\includegraphics[angle=90,width=8.5cm,clip]{3057fig5.ps} \end{figure}$ Figure 5: Collision strengths for the (3s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X.
Open with DEXTER

In the text

$\begin{figure}\par\includegraphics[angle=-90,width=8.5cm,clip]{3057fig12.ps} \end{figure}$ Figure 12: Cross sections for the (2s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X. Continuous curve - present results, broken curve - earlier theoretical results of Tayal (2000), circles - experimental results of Niimura et al. (2002).
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In the text

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig6.ps}\end{figure}$ Figure 6: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s3p⁶ ²S_1/2 (1-3) transition of Fe X.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig7.ps}\end{figure}$ Figure 7: Collision strengths for the 3s²3p⁵ ²P $_{1/2}^{\rm o}$ -3s3p⁶ ²S_1/2 (2-3) transition of Fe X.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig8.ps}\end{figure}$ Figure 8: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s²3p⁴(³P)3d ⁴D_5/2 (1-4) transition of Fe X.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig9.ps}\end{figure}$ Figure 9: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s²3p⁴(³P)3d ⁴D_7/2 (1-5) transition of Fe X.
Open with DEXTER

In the text

$\begin{figure} \par\subfigure[\bf {}]{\includegraphics[angle=-90,width=7.7cm,cli... ...ure[]{\includegraphics[angle=-90,width=7.7cm,clip]{3057fig1b.ps} }\end{figure}$	Figure 1: Partial collision strengths for the (3s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
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$\begin{figure} \par\subfigure[]{\includegraphics[angle=-90,width=8cm,clip]{3057f... ...igure[]{\includegraphics[angle=-90,width=8cm,clip]{3057fig2b.ps} }\end{figure}$	Figure 2: Partial collision strengths for the 3s²3p⁵ ²P $_{3/2}^\circ {-}3$ s3p⁶ ²S_1/2 (1-3) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
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$\begin{figure} \par\subfigure[]{\includegraphics[angle=-90,width=8cm,clip]{3057f... ...igure[]{\includegraphics[angle=-90,width=8cm,clip]{3057fig3b.ps} }\end{figure}$	Figure 3: Partial collision strengths for the 3s3p⁶ ²S _1/2-3s²3p⁴(¹S)3d ²D_5/2 (3-26) transition of Fe X, at three energies of: a) 10 Ryd (circles), 30 Ryd (triangles), and 50 Ryd (stars), and b) 100 Ryd (circles), 150 Ryd (triangles), and 200 Ryd (stars).
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$\begin{figure} \par\includegraphics[angle=-90,width=8cm,clip]{3057fig4.ps} \end{figure}$	Figure 4: Partial sums of collision strengths for the 3s²3p⁵ ²P $_{3/2}^\circ {-}3$ s3p⁶ ²S_1/2 (1-3) transition of Fe X, at three energies of 18 Ryd (circles), 27 Ryd (triangles), and 45 Ryd (stars).
Open with DEXTER

$\begin{figure} \par\includegraphics[angle=90,width=8.5cm,clip]{3057fig5.ps} \end{figure}$	Figure 5: Collision strengths for the (3s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X.
Open with DEXTER

$\begin{figure}\par\includegraphics[angle=-90,width=8.5cm,clip]{3057fig12.ps} \end{figure}$	Figure 12: Cross sections for the (2s²3p⁵) ²P $_{3/2}^\circ {-}^2$ P $_{1/2}^\circ$ (1-2) transition of Fe X. Continuous curve - present results, broken curve - earlier theoretical results of Tayal (2000), circles - experimental results of Niimura et al. (2002).
Open with DEXTER

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig6.ps}\end{figure}$	Figure 6: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s3p⁶ ²S_1/2 (1-3) transition of Fe X.
Open with DEXTER

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig7.ps}\end{figure}$	Figure 7: Collision strengths for the 3s²3p⁵ ²P $_{1/2}^{\rm o}$ -3s3p⁶ ²S_1/2 (2-3) transition of Fe X.
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$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig8.ps}\end{figure}$	Figure 8: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s²3p⁴(³P)3d ⁴D_5/2 (1-4) transition of Fe X.
Open with DEXTER

$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig9.ps}\end{figure}$	Figure 9: Collision strengths for the 3s²3p⁵ ²P $_{3/2}^{\rm o}$ -3s²3p⁴(³P)3d ⁴D_7/2 (1-5) transition of Fe X.
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$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig10.ps}\end{figure}$	Figure 10: Collision strengths for the 3s3p⁶ ²S_1/2-3s²3p⁴(³P)3d ⁴D_5/2 (3-4) transition of Fe X.
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$\begin{figure} \par\includegraphics[angle=90,width=8cm,clip]{3057fig11.ps}\end{figure}$	Figure 11: Collision strengths for the 3s3p⁶ ²S_1/2-3s²3p⁴(³P)3d ⁴D_7/2 (3-5) transition of Fe X.
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