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$\begin{figure} \includegraphics[width=11.5cm,height=8cm]{6809fig1.eps}\end{figure}$ Figure 1: Schematic view of a global acceleration region composed of multiple acceleration regions. The size of one AR is proportional to the value of the magnetic energy coming into the acceleration region. The small grey arrows represent the direction of accelerated electrons in each AR. The grey and white arrows outside the global acceleration region represent, respectively, the accelerated electrons and ions.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,height=6.5cm]{6809fig2.eps}\end{figure}$ Figure 2: Kinetic particle energy distribution obtained for $n_{\rm AR}=10~000$ , $\zeta =5/3$ and with a distribution of particle acceleration length given by a power law of spectral index $\delta =3$ . The temperature of the injected Maxwellian is 10⁶ K.
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In the text

$\begin{figure} \par\includegraphics[width=14cm,height=7cm]{6809fig3.eps}\end{figure}$ Figure 3: Kinetic particle energy distributions obtained for $n_{\rm AR}=10~000$ , $\zeta =1.6$ , and $\delta =3$ . In the left panel, 10% of the total number of particles undergo between 1 and 1000 interactions (dashed line). In the right panel, 10% of the total number of particles undergo between 1 and 10 000 interactions (dashed line). The dash-dotted line represents the thermal part of the spectra.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,height=6.5cm]{6809fig2.eps}\end{figure}$	Figure 2: Kinetic particle energy distribution obtained for $n_{\rm AR}=10~000$ , $\zeta =5/3$ and with a distribution of particle acceleration length given by a power law of spectral index $\delta =3$ . The temperature of the injected Maxwellian is 10⁶ K.
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