Abstract
Four-wave mixing (FWM) in semiconductor laser amplifiers (SLA) is of interest for both theoretical and experimental investigations. Considerable progress has been made towards a better understanding of the basic physical phenomena,1-3 as well as towards applications for fast optical signal processing.4-5 Conventional FWM experiments use a pump wave E1 (frequency ω1) and a signal wave EA (ωA) copropagating with the pump. To efficiently create mixing products, both waves are required to have the same polarization, which is a major drawback for the application of FWM in optical communication networks.
© 1996 Optical Society of America
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