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Line 33: :<math> \frac{1}{\epsilon_r} = \sum_{m=-\infty}^{+\infty} K_m^{\epsilon_r} e^{-ji \frac{2\pi m}{a}z} </math> :<math> E(\omega,\vec{r}) = \sum_{n=-\infty}^{+\infty} K_n^{E_y} e^{-ji\frac{2\pi n}{a}z} e^{-ji\vec{k}\vec{r}} </math>

Plane wave expansion method: Difference between revisions