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$\begin{figure} \par\includegraphics[width=8.2cm,clip]{7260fig1.eps}\end{figure}$ Figure 1: The ratio of perpendicular and parallel diffusion coefficients ( $\kappa _{xx} (t) / \kappa _{zz} (t)$ ) for $R=R_L / l_{\rm slab}=0.001$ . The results from test-particle simulations (dotted line) are compared to various theoretical results: NLGC-theory (dashed line), ENLGC-theory (dash-dotted line), and our GCD-model (solid line).
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In the text

$\begin{figure} \par\includegraphics[width=8.2cm,clip]{7260fig2.eps}\end{figure}$ Figure 2: The parameters $b_{\parallel }$ and $b_{\perp }$ as a function of time for different values of the dimensionless rigidity: R=10^-3 (dotted line), R=10^-2 (dashed line), and R=10^-1 (solid line). The dots denote the values predicted by the GCD-model. Clearly we find a weakly superdiffusive behavior of parallel transport ( $b_{\parallel } > 0$ ) and a weakly subdiffusive behavior of perpendicular transport ( $b_{\perp } < 0$ ).
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In the text

$\begin{figure} \par\includegraphics[width=8.2cm,clip]{7260fig1.eps}\end{figure}$	Figure 1: The ratio of perpendicular and parallel diffusion coefficients ( $\kappa _{xx} (t) / \kappa _{zz} (t)$ ) for $R=R_L / l_{\rm slab}=0.001$ . The results from test-particle simulations (dotted line) are compared to various theoretical results: NLGC-theory (dashed line), ENLGC-theory (dash-dotted line), and our GCD-model (solid line).
Open with DEXTER