All Figures

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig1a}\par\vspace*{5... ...}\par\vspace*{5.5mm} \includegraphics[width=11.05cm,clip]{1783fig1c}\end{figure}$ Figure 1: Albedo and linear polarization as a function of scattering angle for aggregate particles consisting of 128 monomers with radius ${a}_{{\rm m}}=90$ nm and the imaginary part of refractive index k=0.01 ( upper panel), 0.1 ( middle panel), and 1.0 ( lower panel). Solid lines: results at a wavelength $\lambda =450$ nm for particles grown under the ballistic cluster-cluster aggregation (BCCA) process; dotted lines: results at $\lambda =600$ nm for BCCA particles; open circles: results at $\lambda =450$ nm for particles grown under the ballistic particle-cluster aggregation (BPCA) process; crosses: results at $\lambda =600$ nm for BPCA particles.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig5a}\par\vspace*{5... ...5b}\par\vspace*{5mm} \includegraphics[width=11.05cm,clip]{1783fig5c}\end{figure}$ Figure 5: Albedo and linear polarization as a function of scattering angle for an aggregate particle consisting of N=128 monomers with radius ${a}_{{\rm m}}=100$ nm and the real part of refractive index n=1.8 ( upper panel), n=1.9 ( middle panel), and n=2.0 ( lower panel).
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig6}\end{figure}$ Figure 6: The N=128 aggregate consisting of magnesium-rich olivine with the complex refractive index $m=1.69+{{\rm i}}~0.000104$ at a wavelength of $\lambda =450$ nm and $m=1.68+{\rm i}~0.0000115$ at $\lambda =600$ nm.
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In the text

$\begin{figure} \includegraphics[width=11.05cm,clip]{1783fig7}\end{figure}$ Figure 7: The N=128 aggregate consisting of organic refractory with the complex refractive index $m=1.91+{\rm i}~0.317$ at a wavelength of $\lambda =450$ nm and $m=1.97+{\rm i}~0.279$ at $\lambda =600$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig10.eps} % \end{figure}$ Figure 10: Albedo and linear polarization as a function of scattering angle for aggregate particles of 128 monomers composed of a synthetic mixture of magnesium-rich olivine, organic refractory, amorphous carbon, and pyrrhotite. The results are shown with various assumptions for the volume fraction ${f}_{{\rm or}}$ of organic refractory occupying carbonaceous materials.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig11a}\par\vspace*{5mm} \includegraphics[width=11.25cm,clip]{1783fig11b}\end{figure}$ Figure 11: Albedo and linear polarization as a function of scattering angle for aggregate particles composed of a synthetic mixture of amorphous olivine, amorphous carbon, and pyrrhotite ( top). The number of monomers increases from N=4 ( left) to 256 ( right) by doubling the monomer number. The backscatter region for the polarization curve is enlarged in the range of scattering angle between 165 and $180\hbox {$^\circ $ }$ .
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig2a}\par\vspace*{5... ...2b}\par\vspace*{5mm} \includegraphics[width=11.05cm,clip]{1783fig2c}\end{figure}$ Figure 2: The same as Fig. 1, but with radius ${a}_{{\rm m}}=100$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig3a}\par\vspace*{5... ...3b}\par\vspace*{5mm} \includegraphics[width=11.05cm,clip]{1783fig3c}\end{figure}$ Figure 3: The same as Fig. 1, but with radius ${a}_{{\rm m}}=110$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig4a}\par\vspace*{5... ...4b}\par\vspace*{5mm} \includegraphics[width=11.05cm,clip]{1783fig4c}\end{figure}$ Figure 4: The same as Fig. 1, but with radius ${a}_{{\rm m}}=120$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig8}\end{figure}$ Figure 8: The N=128 aggregate consisting of amorphous carbon with the complex refractive index $m=1.95+{\rm i}~0.786$ at a wavelength of $\lambda =450$ nm and $m=2.14+{\rm i}~0.805$ at $\lambda =600$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig9}\end{figure}$ Figure 9: The N=128 aggregate consisting of pyrrhotite with the complex refractive index $m=1.45+{\rm i}~1.53$ at a wavelength of $\lambda =450$ nm and $m=1.70+{\rm i}~1.86$ at $\lambda =600$ nm.
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In the text

$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig5a}\par\vspace{5... ...5b}\par\vspace{5mm} \includegraphics[width=11.05cm,clip]{1783fig5c}\end{figure}$	Figure 5: Albedo and linear polarization as a function of scattering angle for an aggregate particle consisting of N=128 monomers with radius ${a}_{{\rm m}}=100$ nm and the real part of refractive index n=1.8 ( upper panel), n=1.9 ( middle panel), and n=2.0 ( lower panel).
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig6}\end{figure}$	Figure 6: The N=128 aggregate consisting of magnesium-rich olivine with the complex refractive index $m=1.69+{{\rm i}}~0.000104$ at a wavelength of $\lambda =450$ nm and $m=1.68+{\rm i}~0.0000115$ at $\lambda =600$ nm.
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$\begin{figure} \includegraphics[width=11.05cm,clip]{1783fig7}\end{figure}$	Figure 7: The N=128 aggregate consisting of organic refractory with the complex refractive index $m=1.91+{\rm i}~0.317$ at a wavelength of $\lambda =450$ nm and $m=1.97+{\rm i}~0.279$ at $\lambda =600$ nm.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig10.eps} % \end{figure}$	Figure 10: Albedo and linear polarization as a function of scattering angle for aggregate particles of 128 monomers composed of a synthetic mixture of magnesium-rich olivine, organic refractory, amorphous carbon, and pyrrhotite. The results are shown with various assumptions for the volume fraction ${f}_{{\rm or}}$ of organic refractory occupying carbonaceous materials.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig2a}\par\vspace{5... ...2b}\par\vspace{5mm} \includegraphics[width=11.05cm,clip]{1783fig2c}\end{figure}$	Figure 2: The same as Fig. 1, but with radius ${a}_{{\rm m}}=100$ nm.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig3a}\par\vspace{5... ...3b}\par\vspace{5mm} \includegraphics[width=11.05cm,clip]{1783fig3c}\end{figure}$	Figure 3: The same as Fig. 1, but with radius ${a}_{{\rm m}}=110$ nm.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig4a}\par\vspace{5... ...4b}\par\vspace{5mm} \includegraphics[width=11.05cm,clip]{1783fig4c}\end{figure}$	Figure 4: The same as Fig. 1, but with radius ${a}_{{\rm m}}=120$ nm.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig8}\end{figure}$	Figure 8: The N=128 aggregate consisting of amorphous carbon with the complex refractive index $m=1.95+{\rm i}~0.786$ at a wavelength of $\lambda =450$ nm and $m=2.14+{\rm i}~0.805$ at $\lambda =600$ nm.
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$\begin{figure} \par\includegraphics[width=11.05cm,clip]{1783fig9}\end{figure}$	Figure 9: The N=128 aggregate consisting of pyrrhotite with the complex refractive index $m=1.45+{\rm i}~1.53$ at a wavelength of $\lambda =450$ nm and $m=1.70+{\rm i}~1.86$ at $\lambda =600$ nm.
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