All Figures

$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig1a.ps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig1b.ps} } \end{figure}$ Figure 1: Partial collision strengths for the 2s ²S_1/2-2p ²P $^\circ _{1/2}$ (2-3) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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In the text

$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig2a.eps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig2b.eps} } \end{figure}$ Figure 2: Partial collision strengths for the 2s ²S_1/2-3p ²P $^\circ _{1/2}$ (2-5) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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In the text

$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig3a.ps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig3b.eps} } \end{figure}$ Figure 3: Partial collision strengths for the 3s ²S_1/2-3d ²D_3/2 (6-7) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=9cm,clip]{fig4.ps}\end{figure}$ Figure 4: Comparison of collision strengths for the 14-15 (4d ²D_5/2-4f ²F $^\circ _{5/2}$ ), 21-22 (5f ²F $^\circ _{5/2}$ -5d ²D_5/2), and 23-24 (5g ²G_7/2-5f ²F $^\circ _{7/2}$ ) transitions of Fe XXVI. Broken curves are from the CC+CB programs, and the $\Omega$ from FAC are shown as, squares: 14-15, circles: 21-22 and stars: 23-24 transition.
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In the text

$\begin{figure} \par\subfigure[]{\includegraphics[angle=90,width=9cm,clip]{fig5a.... ... \subfigure[]{\includegraphics[angle=90,width=9cm,clip]{fig5b.ps} } \end{figure}$ Figure 5: Collision strengths for the 1s ²S_1/2-2s ²S_1/2 (1-2) transition of Fe XXVI.
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In the text

$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig6.ps}\end{figure}$ Figure 6: Collision strengths for the 1s ²S_1/2-2p ²P $^\circ _{1/2}$ (1-3) transition of Fe XXVI.
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In the text

$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig7.ps}\end{figure}$ Figure 7: Collision strengths for the 2s ²S_1/2-2p ²P $^\circ _{1/2}$ (2-3) transition of Fe XXVI.
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In the text

$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig8.ps}\end{figure}$ Figure 8: Collision strengths for the 2p ²P $^\circ _{1/2}$ -3s ²S_1/2 (3-6) transition of Fe XXVI.
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In the text

$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig1a.ps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig1b.ps} } \end{figure}$	Figure 1: Partial collision strengths for the 2s ²S_1/2-2p ²P $^\circ _{1/2}$ (2-3) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig2a.eps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig2b.eps} } \end{figure}$	Figure 2: Partial collision strengths for the 2s ²S_1/2-3p ²P $^\circ _{1/2}$ (2-5) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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$\begin{figure} \mbox{\includegraphics[angle=-90,width=8.8cm,clip]{fig3a.ps}\hspace{3mm} \includegraphics[angle=-90,width=8.8cm,clip]{fig3b.eps} } \end{figure}$	Figure 3: Partial collision strengths for the 3s ²S_1/2-3d ²D_3/2 (6-7) transition of Fe XXVI, at three energies of: (left panel) 700 Ryd (circles), 800 Ryd (triangles), and 900 Ryd (stars), (right panel) 1100 Ryd (circles), 1300 Ryd (triangles), and 1500 Ryd (stars).
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$\begin{figure} \par\includegraphics[angle=-90,width=9cm,clip]{fig4.ps}\end{figure}$	Figure 4: Comparison of collision strengths for the 14-15 (4d ²D_5/2-4f ²F $^\circ _{5/2}$ ), 21-22 (5f ²F $^\circ _{5/2}$ -5d ²D_5/2), and 23-24 (5g ²G_7/2-5f ²F $^\circ _{7/2}$ ) transitions of Fe XXVI. Broken curves are from the CC+CB programs, and the $\Omega$ from FAC are shown as, squares: 14-15, circles: 21-22 and stars: 23-24 transition.
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$\begin{figure} \par\subfigure[]{\includegraphics[angle=90,width=9cm,clip]{fig5a.... ... \subfigure[]{\includegraphics[angle=90,width=9cm,clip]{fig5b.ps} } \end{figure}$	Figure 5: Collision strengths for the 1s ²S_1/2-2s ²S_1/2 (1-2) transition of Fe XXVI.
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$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig6.ps}\end{figure}$	Figure 6: Collision strengths for the 1s ²S_1/2-2p ²P $^\circ _{1/2}$ (1-3) transition of Fe XXVI.
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$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig7.ps}\end{figure}$	Figure 7: Collision strengths for the 2s ²S_1/2-2p ²P $^\circ _{1/2}$ (2-3) transition of Fe XXVI.
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$\begin{figure} \par\includegraphics[angle=90,width=9cm,clip]{fig8.ps}\end{figure}$	Figure 8: Collision strengths for the 2p ²P $^\circ _{1/2}$ -3s ²S_1/2 (3-6) transition of Fe XXVI.
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