Abstract
A simple and efficient method for computing bandgap structures of two-dimensional photonic crystals is presented. Using the Dirichlet-to-Neumann (DtN) map of the unit cell, the bandgaps are calculated as an eigenvalue problem for each given frequency, where the eigenvalue is related to the Bloch wave vector. A linear matrix eigenvalue problem is obtained even when the medium is dispersive. For photonic crystals composed of a square lattice of parallel cylinders, the DtN map is obtained by a cylindrical wave expansion. This leads to eigenvalue problems for relatively small matrices. Unlike other methods based on cylindrical wave expansions, sophisticated lattice sums techniques are not needed. © 2006 Optical Society of America.
| Original language | English |
|---|---|
| Pages (from-to) | 3217-3222 |
| Journal | Journal of the Optical Society of America A: Optics and Image Science, and Vision |
| Volume | 23 |
| Issue number | 12 |
| DOIs | |
| Publication status | Published - Dec 2006 |
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