$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f1.eps}\end{figure}$ Figure 1: The KAW-like root of MDR $\Omega = \Omega _{1} = \Omega _{1} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f2.eps}\end{figure}$ Figure 2: The SMAW-like root of MDR $\Omega = \Omega _{4} = \Omega _{4} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f3.eps}\end{figure}$ Figure 3: The growth rate of KAW-like instability $\Gamma _{1} = \Gamma \left ( {\Omega _{1}} \right ) = \Gamma _{1} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f4.eps} \end{figure}$ Figure 4: The growth rate of SMAW-like instability $\Gamma _{4} = \Gamma \left ( {\Omega _{4}} \right ) = \Gamma _{4} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f5.eps} \end{figure}$ Figure 5: The inverse KAW-like root of MDR $\Omega = \Omega _{2} = \Omega _{2} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f6.eps}\end{figure}$ Figure 6: The inverse SMAW-like root of MDR $\Omega = \Omega _{3} = \Omega _{3} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f7.eps}\end{figure}$ Figure 7: The growth rate of the inverse KAW-like instability $\Gamma _{2} = \Gamma \left ( {\Omega _{2}} \right ) = \Gamma _{2} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f8.eps}\end{figure}$ Figure 8: The growth rate of inverse SMAW-like instability $\Gamma _{3} = \Gamma \left ( {\Omega _{3}} \right ) = \Gamma _{3} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f1.eps}\end{figure}$	Figure 1: The KAW-like root of MDR $\Omega = \Omega _{1} = \Omega _{1} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f2.eps}\end{figure}$	Figure 2: The SMAW-like root of MDR $\Omega = \Omega _{4} = \Omega _{4} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f3.eps}\end{figure}$	Figure 3: The growth rate of KAW-like instability $\Gamma _{1} = \Gamma \left ( {\Omega _{1}} \right ) = \Gamma _{1} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f4.eps} \end{figure}$	Figure 4: The growth rate of SMAW-like instability $\Gamma _{4} = \Gamma \left ( {\Omega _{4}} \right ) = \Gamma _{4} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 1.7$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f5.eps} \end{figure}$	Figure 5: The inverse KAW-like root of MDR $\Omega = \Omega _{2} = \Omega _{2} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f6.eps}\end{figure}$	Figure 6: The inverse SMAW-like root of MDR $\Omega = \Omega _{3} = \Omega _{3} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f7.eps}\end{figure}$	Figure 7: The growth rate of the inverse KAW-like instability $\Gamma _{2} = \Gamma \left ( {\Omega _{2}} \right ) = \Gamma _{2} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms3594f8.eps}\end{figure}$	Figure 8: The growth rate of inverse SMAW-like instability $\Gamma _{3} = \Gamma \left ( {\Omega _{3}} \right ) = \Gamma _{3} \left ( {z_{\rm i} ,k_{\rm R}} \right )$ at $t_{{\rm bound}} = 3.3$ and $\left ( {\varepsilon _{\rm R}} \right )_{{\rm bound}} = 6.5\times 10^{-5}$ .
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