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k.ladutenko 7 年之前
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共有 1 个文件被更改,包括 2 次插入2 次删除
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      main.tex

+ 2 - 2
main.tex

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