1994
DOI: 10.1016/0038-1098(94)90394-8
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Exciton radiative decay and polaritons in multiquantum wells: quantum-well-to-superlattice crossover

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Cited by 56 publications
(34 citation statements)
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“…In structures with a small number of wells, the spectrum of these collective excitations consists of a discrete number of quasi-stationary (radiative) modes with a re-distributed oscillator strength: the modes can be classified as super-or sub-radiant. 2,3,5 With an increase of the number of wells in the structure, the radiative life-time of the latter decreases, and the lifetime of the former increases. When the number of periods in the structure becomes large enough, the modes of the MQW are more conveniently described in terms of stationary polaritons of infinite periodic structures.…”
Section: Introductionmentioning
confidence: 99%
“…In structures with a small number of wells, the spectrum of these collective excitations consists of a discrete number of quasi-stationary (radiative) modes with a re-distributed oscillator strength: the modes can be classified as super-or sub-radiant. 2,3,5 With an increase of the number of wells in the structure, the radiative life-time of the latter decreases, and the lifetime of the former increases. When the number of periods in the structure becomes large enough, the modes of the MQW are more conveniently described in terms of stationary polaritons of infinite periodic structures.…”
Section: Introductionmentioning
confidence: 99%
“…[23][24][25][26][27] In MQW Bragg structures, where the interwell distance amounts to half the optical wavelength at the exciton resonance, superradiant coupling was predicted 28,29 and observed [30][31][32] in reflection and degenerate four-wave-mixing ͑DFWM͒ experiments as a collective quantum-well effect mediated by the optical field. At other periodicities the light coupling was predicted 33,34 and observed 20,35,36 to give rise to polaritonic eigenmodes in nonresonant photoluminescence, reflection, transmission, and RRS. Signatures of the modes were also observed in DFWM experiments.…”
Section: Introductionmentioning
confidence: 95%
“…(36), (37) and (39) to derive (a, f )-representation for T . The dispersion equation following from this representation has a relatively simple form:…”
Section: Off-bragg Structuresmentioning
confidence: 99%