$\begin{figure} \par\includegraphics[width=8.5cm]{nonaxi1.ps}\par\end{figure}$ Figure 1: The dependence of $\Gamma ^2$ on q for B_z=0 and m=1. Numbers near the curves indicate the values of parameter $\alpha$ .
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In the text

$\begin{figure} \par\includegraphics[width=9cm]{nonaxi2.ps}\par\end{figure}$ Figure 2: The dependence of $\Gamma ^2$ on q for $\varepsilon = B_z/ B_{\varphi 0}= 0.1$ and m=1. Numbers near the curves correspond to values of $\alpha$ .
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In the text

$\begin{figure} \par\includegraphics[width=9cm]{nonaxi3.ps}\par\end{figure}$ Figure 3: The dependence of $\Gamma ^2$ on q for $\varepsilon = B_z/ B_{\varphi 0}= 0.1$ , $\alpha = 0$ , anddifferent values of m. Solid, long-dashed, dotted, short-dashed, anddot-dashed lines are for m=0,1,2,3,4, respectively.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm]{nonaxi8.ps}\par\end{figure}$ Figure 8: The critical value of $\alpha$ that determines the onset of instability as a function of $\varepsilon$ for |q| = 10. Solid and dashed curves correspond to q=10 and q=-10, respectively. The dash-and-dotted curve show critical $\alpha$ for m=0, which does not depend on the sign of q.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm]{nonaxi1.ps}\par\end{figure}$	Figure 1: The dependence of $\Gamma ^2$ on q for B_z=0 and m=1. Numbers near the curves indicate the values of parameter $\alpha$ .
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$\begin{figure} \par\includegraphics[width=9cm]{nonaxi2.ps}\par\end{figure}$	Figure 2: The dependence of $\Gamma ^2$ on q for $\varepsilon = B_z/ B_{\varphi 0}= 0.1$ and m=1. Numbers near the curves correspond to values of $\alpha$ .
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$\begin{figure} \par\includegraphics[width=9cm]{nonaxi3.ps}\par\end{figure}$	Figure 3: The dependence of $\Gamma ^2$ on q for $\varepsilon = B_z/ B_{\varphi 0}= 0.1$ , $\alpha = 0$ , anddifferent values of m. Solid, long-dashed, dotted, short-dashed, anddot-dashed lines are for m=0,1,2,3,4, respectively.
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$\begin{figure} \par\includegraphics[width=9cm]{nonaxi4.ps}\par\end{figure}$	Figure 4: The same as in Fig. 3 but for $B_z/B_{\varphi 0}=0.5$ .
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$\begin{figure} \par\includegraphics[width=9cm]{nonaxi5.ps}\par\end{figure}$	Figure 5: The same as in Fig. 3 but for $\alpha = 1$ .
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$\begin{figure} \par\includegraphics[width=9cm]{nonaxi6.ps}\par\end{figure}$	Figure 6: The same as in Fig. 3 but for $\alpha = 2$ . The dash-dot-dotted line represents m=10.
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$\begin{figure} \par\includegraphics[width=8.5cm]{nonaxi7.ps}\par\end{figure}$	Figure 7: The same as in Fig. 3 but for $\alpha =-0.5$ .
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$\begin{figure} \par\includegraphics[width=8.5cm]{nonaxi8.ps}\par\end{figure}$	Figure 8: The critical value of $\alpha$ that determines the onset of instability as a function of $\varepsilon$ for \|q\| = 10. Solid and dashed curves correspond to q=10 and q=-10, respectively. The dash-and-dotted curve show critical $\alpha$ for m=0, which does not depend on the sign of q.
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