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@@ -534,8 +534,8 @@ license.
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intensity in the front side of the nanoparticle to that in the back
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side normalized to their sum:
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$G_I = (I^{front}-I^{back})/(I^{front}+I^{back})$, where
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- $I^{front}=\int_{(z>0)}|E(z)|^2dv$ and
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- $I^{back}=\int_{(z<0)} |E(z)|^2dv$. Fig.~\ref{mie-fdtd}(b)
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+ $I^{front}=\int_{(z>0)}|E|^2d{\mathrm{v}}$ and
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+ $I^{back}=\int_{(z<0)} |E|^2d{\mathrm{v}}$. Fig.~\ref{mie-fdtd}(b)
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shows the $G$ factor as a function of the nanoparticle size. For the
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nanoparticles of sizes below the first magnetic dipole resonance, the
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intensity is enhanced in the front side as in Fig. \ref{mie-fdtd}(c)
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