Figure 3.

Enhancement factor dependence on optical properties. The enhancement factor appears to be approximately proportional to $L_{\mathrm{sc}}{\mu }_s^{*}$ and weakly dependent on g (a) and m (b). However, when the proportionality coefficient [$C_E=E∕\left(L_{\mathrm{sc}}{\mu }_s^{*}\right)$] is plotted, variations with g (c) and m (d) become apparent. These variations are attributed to the variation in the sharp peak of P(r) at small radial distances.