1999
DOI: 10.1002/(sici)1521-3951(199909)215:1<199::aid-pssb199>3.0.co;2-t
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Exciton Polaritons in Periodic Nanostructures

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Cited by 29 publications
(18 citation statements)
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“…29,30 The structures are multiple quantum wells separated by wide-gap semiconductor barriers. The width, d, of each barrier was assumed to be close to λ 0 /2, where λ 0 is the wavelength corresponding to the intra-well exciton resonance frequency, ω T .…”
Section: Discussionmentioning
confidence: 99%
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“…29,30 The structures are multiple quantum wells separated by wide-gap semiconductor barriers. The width, d, of each barrier was assumed to be close to λ 0 /2, where λ 0 is the wavelength corresponding to the intra-well exciton resonance frequency, ω T .…”
Section: Discussionmentioning
confidence: 99%
“…The condition d ≈ λ 0 /2 implies that the Bragg frequency, ω B is close to ω T . Since the quantum wells with strong frequency dispersion at ω ∼ ω T had thickness much smaller than d, then a real Bragg gap in the structures 29,30 was lacking. However, under the condition ω T ≡ ω B the dispersion law of light propagating along the principal axis was shown to have a gap within a frequency range |ω − ω T | = (2Γ 0 ω T /π) 1/2 = Ω (eff) .…”
Section: Discussionmentioning
confidence: 99%
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“…Согласно теории [21,36,37], для брэгговской струк-туры с квантовыми ямами ширина спектра экситонно-го отражения света R …”
Section: численный анализ и обсуждениеunclassified
“…In this case the reflection from and transmission through a QW layer is well described by one-pole functions of the light frequency (see, e.g., the review [2]). Then the amplitude reflection coefficient for the whole system can be presented in the convenient form…”
mentioning
confidence: 99%