Optical properties of photonic crystals - New Jersey Institute of ...
Optical properties of photonic crystals - New Jersey Institute of ...
Optical properties of photonic crystals - New Jersey Institute of ...
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Figure 3.4 Right-hand side, the electromagnetic dispersion forbidden gap at the wave<br />
vector <strong>of</strong> the periodicity. Left-hand side, the electron wave dispersion typical <strong>of</strong> a directgap<br />
semiconductor ¹º<br />
In the above figure 3.4, the dots represent electrons and holes. Since the<br />
<strong>photonic</strong> band gap straddles the electronic band edge, electron hole recombination<br />
into photons is inhibited. The photons have no place to go¹º. One <strong>of</strong> the most<br />
important applications <strong>of</strong> this spontaneous emission inhibition is the enhancement<br />
<strong>of</strong> photon-number-state squeezing, which plays an important role in quantum<br />
optics.<br />
The conventional method to convert optical energy into electrical signals could be<br />
described as follows. Effective photovoltaic material must absorb light to generate a<br />
mobile charge and to move that charge by means <strong>of</strong> a built-in electric potential. It was<br />
discovered in the 1830s that exposing an electrolytic cell to light increased the amount <strong>of</strong>