2000
DOI: 10.1103/physrevlett.85.5392
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Quantum Correlations in the Nonperturbative Regime of Semiconductor Microcavities

Abstract: The nonlinear optical response of semiconductor microcavities in the nonpertubative regime is studied in resonant single-beam-transmission and pump-probe experiments. In both cases a pronounced third transmission peak lying spectrally between the two normal modes is observed. A fully quantized theory is essential for the agreement with the experimental observations, demonstrating that quantum fluctuations leading to intraband polarizations are responsible for this effect.

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Cited by 35 publications
(25 citation statements)
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“…More intuitively, DJ q; k describes correlations between an intraband carrier density and a photon. This carrier-photon entanglement has proven important already in our previous quantum-optical investigations [5,6].…”
mentioning
confidence: 89%
See 1 more Smart Citation
“…More intuitively, DJ q; k describes correlations between an intraband carrier density and a photon. This carrier-photon entanglement has proven important already in our previous quantum-optical investigations [5,6].…”
mentioning
confidence: 89%
“…While most aspects of the semiclassical regime are well understood [4], quantum-optical features are emerging only gradually. In former publications, we have already presented and analyzed cases where quantum-optical features have led to surprising results in traditional pump-probe experiments [5,6]. These investigations were crucial first steps in developing semiconductor systems towards quantumoptical applications.…”
mentioning
confidence: 93%
“…(8) and the definitions Eq. (6) we get the following expressions for the electronic correlation functions: 4c 11 qq 0 ðtÞ ¼ hP I q k ðtÞP q 0 k i þ hP I q k ðtÞP þ q 0 k i þ hP þI q k ðtÞP q 0 k i þ hP þI q k ðtÞP þ q 0 k i, 4c 12 qq 0 ðtÞ ¼ À ihP I q k ðtÞP q 0 k i þ ihP I q k ðtÞP þ q 0 k i À ihP þI q k ðtÞP q 0 k i þ ihP þI q k ðtÞP þ q 0 k i, 4c 21 qq 0 ðtÞ ¼ À ihP I q k ðtÞP q 0 k i À ihP I q k ðtÞP þ q 0 k i þ ihP þI q k ðtÞP q 0 k i þ ihP þI q k ðtÞP þ q 0 k i, 4c 22 qq 0 ðtÞ ¼ À hP I q k ðtÞP q 0 k i þ hP I q k ðtÞP þ q 0 k i þ hP þI q k ðtÞP q 0 k i À hP þI q k ðtÞP þ q 0 k i.…”
Section: Appendix B the Correlation Functionsmentioning
confidence: 99%
“…The coherent part of the equations constitutes the well-known semiconductor Bloch equations [5], while the incoherent part leads to the semiconductor luminescence [4,6]. The coupling between coherent and incoherent dynamics, made possible by the quantized light field, leads to interesting quantum-optical effects in seemingly classical experiments [7,8] and to coherent control of incoherently emitted light [9]. Moreover, the theory has interesting implications for the interpretation of luminescence signals in connection with exciton formation [10,11].…”
Section: Introductionmentioning
confidence: 96%
“…The correct three-dimensional treatment of the cavity mode leads to a structured continuum of guided modes that can have an influence on the luminescence, 56 and plays an important role in the observation of a quantum-fluctuation-induced third peak in the pump-probe spectrum of microcavities. 57 In Fig. 12͑a͒ RRS signals are shown that have been computed for a microcavity consisting of a spacer embedded in ten and 12.5 pairs of distributed Bragg reflectors.…”
Section: Microcavitymentioning
confidence: 99%