Abstract
The nonlinear optical response of semiconductor microcavities in the nonperturbative regime has been the subject of many recent experiments. Contrary to clear demonstrations of the quantized nature of the vacuum-field Rabi splitting of a single atom, most of the experiments on semiconductor microcavities could be explained in terms of a classical light field. Only recently, quan-tized light field effects have been reported in a coherent control experiment1 and theoretically investigated in secondary emission.2
© 2001 Optical Society of America
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