$\begin{figure} \par\epsfig{file=0304fig1.eps, width=8.5cm,clip=} \end{figure}$ Figure 1: The momentum diffusion coefficient for shear Alfvén waves ${A}^{\rm A}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig2.eps, width=8.5cm,clip=} \end{figure}$ Figure 2: The momentum diffusion coefficient for fast magnetosonic waves $A^{\rm F}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig3.eps, width=8.5cm,clip=} \end{figure}$ Figure 3: The parallel spatial diffusion coefficient for shear Alfvén waves $\kappa ^{\rm A}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig4.eps, width=8.5cm,clip=} \end{figure}$ Figure 4: The parallel spatial diffusion coefficient for fast magnetosonic waves ${\kappa }^{\rm F}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig5.eps, width=8.5cm,clip=} \end{figure}$ Figure 5: The parallel mean free path for shear Alfvén waves $\lambda ^{\rm A}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig6.eps, width=8.5cm,clip=} \end{figure}$ Figure 6: The parallel mean free path for fast magnetosonic waves $\lambda ^{\rm F}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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In the text

$\begin{figure} \par\epsfig{file=0304fig1.eps, width=8.5cm,clip=} \end{figure}$	Figure 1: The momentum diffusion coefficient for shear Alfvén waves ${A}^{\rm A}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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$\begin{figure} \par\epsfig{file=0304fig2.eps, width=8.5cm,clip=} \end{figure}$	Figure 2: The momentum diffusion coefficient for fast magnetosonic waves $A^{\rm F}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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$\begin{figure} \par\epsfig{file=0304fig3.eps, width=8.5cm,clip=} \end{figure}$	Figure 3: The parallel spatial diffusion coefficient for shear Alfvén waves $\kappa ^{\rm A}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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$\begin{figure} \par\epsfig{file=0304fig4.eps, width=8.5cm,clip=} \end{figure}$	Figure 4: The parallel spatial diffusion coefficient for fast magnetosonic waves ${\kappa }^{\rm F}$ for protons (solid lines), electrons and positrons (dashedlines). We show the results for different values of the anisotropyparameter $\Lambda$ .
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$\begin{figure} \par\epsfig{file=0304fig5.eps, width=8.5cm,clip=} \end{figure}$	Figure 5: The parallel mean free path for shear Alfvén waves $\lambda ^{\rm A}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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$\begin{figure} \par\epsfig{file=0304fig6.eps, width=8.5cm,clip=} \end{figure}$	Figure 6: The parallel mean free path for fast magnetosonic waves $\lambda ^{\rm F}$ for protons (solid lines), electrons and positrons (dashed lines). We show the results for different values of the anisotropy parameter $\Lambda$ .
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