$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg1a.eps}\vspace*{2mm} \includegraphics[width=8cm,clip]{4141fg1b.eps}\end{figure}$ Figure 1: Damping rate as a function of wavenumber for a) slow-mode waves and b) fast-mode waves, for n₀= 1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀= 2.0 $\times$ $10^6~{\rm K}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg2a.eps}\vspace*{2mm} \includegraphics[width=8cm,clip]{4141fg2b.eps}\end{figure}$ Figure 2: Damping rate as a function of wavenumber for a) slow-mode waves and b) fast-mode waves, for n₀= 1.0 $\times$ $10^{9}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀= 2.0 $\times$ $10^6~{\rm K}$ .
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In the text

$\begin{figure} \par\includegraphics[width=6.8cm,clip]{4141fg3a.eps}\hspace*{2mm}... ...c.eps}\hspace*{2mm} \includegraphics[width=6.8cm,clip]{4141fg3d.eps}\end{figure}$ Figure 3: Damping rate as a function of wavenumber with n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}$ and $B_0=100~{\rm G}$ for a) slow-mode waves, b) fast-mode waves for T₀=3.0 $\times$ $10^6~{\rm K}$ , c) slow-mode waves with different background temperatures, and d) fast-mode waves with different background temperatures.
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg4a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg4b.eps}\end{figure}$ Figure 4: Damping rate as a function of wavenumber with n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}$ and T₀=2.0 $\times$ $10^6~{\rm K}$ for a) fast-mode waves for $B_0=150~{\rm G}$ and b) fast-mode waves with different background magnetic fields.
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg5a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg5b.eps}\end{figure}$ Figure 5: Damping rate as a function of wavenumber with modern viscosity and thermal conductivity for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀=2.0 $\times$ $10^6~{\rm K}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg6a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg6b.eps}\end{figure}$ Figure 6: Damping rate as a function of wavenumber with viscosity and thermal conductivity for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀=2.0 $\times$ $10^6~{\rm K}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg7a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg7b.eps}\end{figure}$ Figure 7: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0=300~{\rm G}, T_0=3.5$ $\times$ $10^6~{\rm K}$ , and L=1.0 $\times$ $10^9~{\rm cm}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg8a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg8b.eps}\end{figure}$ Figure 8: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=3.0 $\times$ $10^9~{\rm cm^{-3}}, B_0=150~{\rm G}, T_0=3.0$ $\times$ $10^6~{\rm K}$ , and L=3.0 $\times$ $10^9~{\rm cm}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg9a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg9b.eps}\end{figure}$ Figure 9: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^9~{\rm cm^{-3}}, B_0=50~{\rm G}, T_0=2.5$ $\times$ $10^6~{\rm K}$ , and L=1.0 $\times$ $10^{10}~{\rm cm}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg1a.eps}\vspace*{2mm} \includegraphics[width=8cm,clip]{4141fg1b.eps}\end{figure}$	Figure 1: Damping rate as a function of wavenumber for a) slow-mode waves and b) fast-mode waves, for n₀= 1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀= 2.0 $\times$ $10^6~{\rm K}$ .
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg2a.eps}\vspace*{2mm} \includegraphics[width=8cm,clip]{4141fg2b.eps}\end{figure}$	Figure 2: Damping rate as a function of wavenumber for a) slow-mode waves and b) fast-mode waves, for n₀= 1.0 $\times$ $10^{9}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀= 2.0 $\times$ $10^6~{\rm K}$ .
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$\begin{figure} \par\includegraphics[width=6.8cm,clip]{4141fg3a.eps}\hspace{2mm}... ...c.eps}\hspace{2mm} \includegraphics[width=6.8cm,clip]{4141fg3d.eps}\end{figure}$	Figure 3: Damping rate as a function of wavenumber with n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}$ and $B_0=100~{\rm G}$ for a) slow-mode waves, b) fast-mode waves for T₀=3.0 $\times$ $10^6~{\rm K}$ , c) slow-mode waves with different background temperatures, and d) fast-mode waves with different background temperatures.
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg4a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg4b.eps}\end{figure}$	Figure 4: Damping rate as a function of wavenumber with n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}$ and T₀=2.0 $\times$ $10^6~{\rm K}$ for a) fast-mode waves for $B_0=150~{\rm G}$ and b) fast-mode waves with different background magnetic fields.
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg5a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg5b.eps}\end{figure}$	Figure 5: Damping rate as a function of wavenumber with modern viscosity and thermal conductivity for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀=2.0 $\times$ $10^6~{\rm K}$ .
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg6a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg6b.eps}\end{figure}$	Figure 6: Damping rate as a function of wavenumber with viscosity and thermal conductivity for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0= 100~{\rm G}$ , and T₀=2.0 $\times$ $10^6~{\rm K}$ .
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg7a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg7b.eps}\end{figure}$	Figure 7: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^{10}~{\rm cm^{-3}}, B_0=300~{\rm G}, T_0=3.5$ $\times$ $10^6~{\rm K}$ , and L=1.0 $\times$ $10^9~{\rm cm}$ .
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg8a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg8b.eps}\end{figure}$	Figure 8: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=3.0 $\times$ $10^9~{\rm cm^{-3}}, B_0=150~{\rm G}, T_0=3.0$ $\times$ $10^6~{\rm K}$ , and L=3.0 $\times$ $10^9~{\rm cm}$ .
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$\begin{figure} \par\includegraphics[width=8cm,clip]{4141fg9a.eps}\vspace*{3mm} \includegraphics[width=8cm,clip]{4141fg9b.eps}\end{figure}$	Figure 9: Variation of damping rate with parameter f for a) slow-mode waves and b) fast-mode waves for n₀=1.0 $\times$ $10^9~{\rm cm^{-3}}, B_0=50~{\rm G}, T_0=2.5$ $\times$ $10^6~{\rm K}$ , and L=1.0 $\times$ $10^{10}~{\rm cm}$ .
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