Abstract
Nonlinear optical properties of quantum wells (QW’s) and superlattices (SL’s) 1,2 are attracting increasing interest. Calculations and observations of strong third-order nonlinearities were reported in GaAs-GaAlAs QW and SL structures. Among the phenomena mentioned as leading to large values of x(3) in such structures are conduction band nonparabolicity 3,4, exciton line saturation 5 and the quantum confined Stark effect (QCSE) 6,7. Practical devices using QCSE, the so-called self-electrooptic effect devices, or SEED’s have been successfully demonstrated 8.
© 1988 Optical Society of America
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