$\begin{figure*} \par\includegraphics[width=12cm,clip]{0792fig2.eps} \end{figure*}$ Figure 2: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{0792fig3.eps} \end{figure}$ Figure 3: Maximum growth rates versus the cutoff energy $E_{\rm c}$ : O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=12cm,clip]{0792fig4.eps} \end{figure}$ Figure 4: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=12cm,clip]{0792fig5.eps} \end{figure}$ Figure 5: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{0792fig6.eps} \end{figure}$ Figure 6: Plots maximum growth rates versus the mirror ratio $\sigma$ : O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{0792fig1.eps} \end{figure}$	Figure 1: Lower-energy cutoff behaviors of power-law electrons with spectrum index $\alpha =3$ .
Open with DEXTER

$\begin{figure} \par\includegraphics[width=12cm,clip]{0792fig2.eps} \end{figure}$	Figure 2: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8cm,clip]{0792fig3.eps} \end{figure}$	Figure 3: Maximum growth rates versus the cutoff energy $E_{\rm c}$ : O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=12cm,clip]{0792fig4.eps} \end{figure}$	Figure 4: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=12cm,clip]{0792fig5.eps} \end{figure}$	Figure 5: Peak growth rates driven by the ECM instability: O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{0792fig6.eps} \end{figure}$	Figure 6: Plots maximum growth rates versus the mirror ratio $\sigma$ : O₁, fundamental waves in the O mode; O₂, harmonic waves in the O mode; X₁, fundamental waves in the X mode; X₂, harmonic waves in the X mode.
Open with DEXTER