Artificial periodically microstructured materials have attracted widespread interest in recent
years because they offer an exciting new way to control the propagation of light. Such periodic
materials, known as photonic crystals, can exhibit full photonic band gaps, that is, energy gaps of
zero density of states. Electromagnetic waves with frequencies in the band gap cannot propagate
through the crystal. Modifying the band gap structure, for instance, by introducing a defect or
arrays of defects, produces effects similar to what can be done by doping electronic
semiconductors. With this picture in mind, photonic crystals are to electromagnetic waves what
semiconductors are to electrons. The purpose of this talk is to present an overview on how things
work in a world ruled by Maxwell equations and Floquet-Bloch theorem, stressing analogies and
differences between quantum mechanics of natural crystals and electromagnetism of artificial
periodic dielectric media.
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