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physica status solidi (b)

Signatures of Quantum Correlations in a Semiconductor Microcavity

Peter Brick, Claudia Ell, M. H�bner, Ove Lyngnes, G. Khitrova, H. M. Gibbs, M. Kira, F. Jahnke, S. W. Koch

Published Sep 1, 2000• 0 citations
Publisher

Abstract

Semiconductor microcavities are studied by resonant single-beam and pump–probe experiments. A third transmission peak in the nonperturbative regime is observed, lying spectrally between the two normal modes. Its dependence on the pulse intensity, pump–probe delay, and pulse polarization is discussed. This intriguing effect is caused by intraband correlations induced by quantum fluctuations.

DOI
10.1002/1521-3951(200009)221:1<107::aid-pssb107>3.0.co;2-5

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physica status solidi (a)•Mar 1, 2000•0 citations
Semiconductor microcavities are studied by resonant single-beam and pump–probe experiments. A third transmission peak in the nonperturbative regime is observed, lying spectrally between the two normal modes. Its dependence on the pulse intensity, pump–probe delay, and pulse polarization is discussed. This intriguing effect is caused by intraband correlations induced by quantum fluctuations.
Summary form only given. 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 semi-conductor microcavities could be explained in terms of a classical light field. Only recently, quantized light field effects have been reported in a coherent control experiment (Lee et al, 1999) and theoretically investigated in secondary emission (Kira et al, 1999). Here, results are presented that display a pronounced third transmission maximum lying energetically between the two normal modes. The third peak can be observed in resonant femtosecond single-beam as well as picosecond pump-probe experiments under various excitation conditions.
A fully quantized theory of optical interactions with semiconductors reveals quantum correlations between the field and carrier density. These quantum correlations lead to intraband coherences which live much longer than the interband dephasing time; the correlations are observed as oscillations in the time-resolved reflectivity in a pump-probe experiment on a normal-mode microcavity. Coherent control of the microcavity normal modes using phase-locked pump pulses enables considerable enhancement of the intraband oscillations due to quantum interference; the detailed phase dependence is well reproduced by the theory.
Summary form only given. We demonstrate that quantum correlations between the cavity field and the carrier density in an InGaAs quantum-well (QW) microcavity can be observed in a novel pump-probe experiment. In our investigations, the lower normal mode of a microcavity is excited with a pair of identical phase-locked pump pulses near normal incidence. The transient reflectivity of a weak probe pulse tuned to the upper normal mode is measured. We will show that long-lived oscillations are observed, which originate in the pump-induced quantum correlations, and that the phase and amplitude of the coherences can be controlled via the relative phase of the pump pulses.
The normal modes in a nonperturbatively coupled quantum-well semiconductor microcavity are linear superpositions of the QW exciton and cavity mode when the QW exciton transition is resonant with the cavity mode. When the lower normal mode is excited by a phase-locked pair of optical pulses, the nonlinear response of a probe pulse tuned to the upper mode is controlled. Thus the normal modes are coupled in their nonlinear optical response due to the nonlinearity of the exciton underlying the two normal modes. The cavity enhancement of the excitonic nonlinearity gives rise to a large signal; modulating the relative phase of the excitation pulses produces a differential reflectivity of up to 10%. Besides the coherent control of normal modes which is explainable with in the frame of semiclassical models, we observe a purely quantum mechanical phenomenon in our system. The quantum correlations between the field and carrier density lead to intraband coherences which live much longer than the interband dephasing time.