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$\begin{figure} \includegraphics[width=4cm,clip]{Fe162_f1a}\includegraphics[width=4cm,clip]{Fe162_f1b}\includegraphics[width=4cm,clip]{Fe162_f1c} \end{figure}$ Figure 1: The geometric albedo ${A}_{\rm p}$ and polarization P for randomly oriented BCCA particles consisting of optically dark submicron grains. The geometric albedo is also described using the corresponding values for S₁₁/k² where S₁₁ and k denote the (1,1) element of the scattering matrix S_ij and the wave number, respectively. Solid lines are the numerical results for the wavelength $\lambda=0.45~\mu$ m and dotted lines are those for $\lambda=0.60~\mu$ m. Dashed horizontal straight lines in the upper left corner of each lower panel are plotted to illustrate P=0. The number of constituentparticles in the aggregate is set to be N=64 (left panel), 128 (middle panel), or 256 (right panel).
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In the text

$\begin{figure} \par\includegraphics[width=4cm,clip]{Fe162_f2a}\includegraphics[width=4cm,clip]{Fe162_f2b}\includegraphics[width=4cm,clip]{Fe162_f2c} \end{figure}$ Figure 2: Same as Fig. 1, but for BPCA particles.
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In the text

$\begin{figure} \par\includegraphics[width=4cm,clip]{Fe162_f2a}\includegraphics[width=4cm,clip]{Fe162_f2b}\includegraphics[width=4cm,clip]{Fe162_f2c} \end{figure}$	Figure 2: Same as Fig. 1, but for BPCA particles.
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