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$\begin{figure} \par\includegraphics[width=12.8cm,clip]{1494fig1.eps}\end{figure}$ Figure 1: Schematic view of the inhomogeneous background configuration and the directions of wave propagation (polarization).
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In the text

$\begin{figure} \par\includegraphics[width=12.3cm,clip]{1494fig2.eps}\end{figure}$ Figure 2: The profiles of the equilibrium quantities plotted against dimensionless x/L_x coordinate: density (panel A)), pressure (panel B)), the magnetic field (panel C)) and plasma beta (panel D)).
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In the text

$\begin{figure} \par\includegraphics[width=16.2cm,clip]{1494fig3.eps}\end{figure}$ Figure 3: Sample solutions of the standing fast magnetosonic modes. Panel A) zeroth-order harmonic n=0, period T=5.6069 min, $\alpha =0.015$ ; Panel B) second-order harmonic n=2, period T=1.8514 min, $\alpha =0.03$ .
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In the text

$\begin{figure} \includegraphics[width=13cm,clip]{1494fig4.eps}\end{figure}$ Figure 4: Results of numerical simulations for the standing fast magnetosonic mode, shown on panel A in Fig. 3. Panel A $_{\bf 1}$ ) the curves of F₁ (Eq. (42)) (solid line) and F₂(Eq. (43)) (dotted line) vs. fractional distance x/L_x for the zeroth-order standing fast mode n=0 and the standing Alfvén mode with m=3; panel B $_{\bf 1}$ ) the numerical solution of the Alfvén mode m=3 amplitude at location $x/L_x\approx x_{0,4}/L_x=0.0767$ ; panel C₁) the numerical solution for mode m=3 at $x/L_x\approx x_{0,3}/L_x=0.7967$ ; panel A $_{\bf 2}$ ) as in panel A $_{\bf 1}$ ) for mode m=4; panel B $_{\bf 2}$ ) as in panel B $_{\bf 1}$ ) for mode m=4; panel C $_{\bf 2}$ ) as in panel C₁) for mode m=4.
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In the text

$\begin{figure} \par\includegraphics[width=13cm,clip]{1494fig5.eps}\end{figure}$ Figure 5: As in Fig. 4 for the second-order harmonic of the fast magnetosonic mode shown on Panel B in Fig. 3 (n=2) and the standing Alfvén with m=8 and m=10. The numerical solutions respectively are given at distances $x_1/L_x \approx x_{2,10}/L_x = 0.6000$ (panels B $_{\bf 1}$ ) and B $_{\bf 2}$ )), $x_2/L_x \approx x_{2,8}/L_x=0.9933$ (panels C $_{\bf 1}$ ) and C $_{\bf 2}$ )). Dashed line in panel A $_{\bf 1}$ ) is curve of F₁ (42) corresponding to the mode m=9.
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In the text

$\begin{figure} \par\includegraphics[width=12.5cm,clip]{1494fig6.eps}\end{figure}$ Figure 6: As in Fig. 5 for the standing Alfvén modes with m=11 and m=12 at respective resonant points $x_1/L_x \approx x_{2,12}/L_x = 0.1033$ (panels B $_{\bf 1}$ ) and B $_{\bf 2}$ )), $x_2/L_x \approx x_{2,11}/L_x=0.3633$ (panels C $_{\bf 1}$ ) and C $_{\bf 2}$ )).
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In the text

$\begin{figure} \par\includegraphics[width=12.8cm,clip]{1494fig1.eps}\end{figure}$	Figure 1: Schematic view of the inhomogeneous background configuration and the directions of wave propagation (polarization).
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$\begin{figure} \par\includegraphics[width=12.3cm,clip]{1494fig2.eps}\end{figure}$	Figure 2: The profiles of the equilibrium quantities plotted against dimensionless x/L_x coordinate: density (panel A)), pressure (panel B)), the magnetic field (panel C)) and plasma beta (panel D)).
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$\begin{figure} \par\includegraphics[width=16.2cm,clip]{1494fig3.eps}\end{figure}$	Figure 3: Sample solutions of the standing fast magnetosonic modes. Panel A) zeroth-order harmonic n=0, period T=5.6069 min, $\alpha =0.015$ ; Panel B) second-order harmonic n=2, period T=1.8514 min, $\alpha =0.03$ .
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$\begin{figure} \par\includegraphics[width=12.5cm,clip]{1494fig6.eps}\end{figure}$	Figure 6: As in Fig. 5 for the standing Alfvén modes with m=11 and m=12 at respective resonant points $x_1/L_x \approx x_{2,12}/L_x = 0.1033$ (panels B $_{\bf 1}$ ) and B $_{\bf 2}$ )), $x_2/L_x \approx x_{2,11}/L_x=0.3633$ (panels C $_{\bf 1}$ ) and C $_{\bf 2}$ )).
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