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Volumn 80, Issue 20, 2009, Pages

Phonon-assisted transitions from quantum dot excitons to cavity photons

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EID: 77954702590     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.201311     Document Type: Article
Times cited : (138)

References (34)
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    • The small discrepancies between the quantum-kinetic and rate-equation simulations are attributed to the too small number of about hundred phonon modes in our simulation, which induce artificial phonon revivals in the simulated decay transients
    • The small discrepancies between the quantum-kinetic and rate-equation simulations are attributed to the too small number of about hundred phonon modes in our simulation, which induce artificial phonon revivals in the simulated decay transients.
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    • The PL spectra were recorded with relatively strong excitation levels (∼10 W/ cm2 ) in order to clearly observe the cavity mode, whilst the time-resolved measurements presented later were performed with much weaker excitation power (≤1 W/ cm2 ) in order to avoid state filling effects
    • The PL spectra were recorded with relatively strong excitation levels (∼ 10 W / cm 2) in order to clearly observe the cavity mode, whilst the time-resolved measurements presented later were performed with much weaker excitation power (≤ 1 W / cm 2) in order to avoid state filling effects.
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    • This is inevitable for these systems since the L3 cavity axis was not intentionally aligned with the [110] crystal axis and the neutral exciton consists of a linearly polarized doublet with a fine-structure splitting below our spectral resolution of 60 μeV
    • This is inevitable for these systems since the L3 cavity axis was not intentionally aligned with the [110] crystal axis and the neutral exciton consists of a linearly polarized doublet with a fine-structure splitting below our spectral resolution of 60 μ eV.
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