2001
DOI: 10.1103/physrevb.63.155307
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Acoustic phonon broadening mechanism in single quantum dot emission

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Cited by 486 publications
(458 citation statements)
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“…A broad shoulder to the quantum dot line shape due to phonons has also been observed in CW-photoluminescence measurements. 25,26 In the case of the ideal two-level atom, the 3p -peak has a slight arrow-head like shape. The exciton-phonon interaction appears to accentuate the arrow-head.…”
Section: Influence Of Detuningmentioning
confidence: 99%
“…A broad shoulder to the quantum dot line shape due to phonons has also been observed in CW-photoluminescence measurements. 25,26 In the case of the ideal two-level atom, the 3p -peak has a slight arrow-head like shape. The exciton-phonon interaction appears to accentuate the arrow-head.…”
Section: Influence Of Detuningmentioning
confidence: 99%
“…This value increases only by a few µeV as the temperature is raised to 30 K. The main effect of the temperature increase on the emission lines is the strong deviation from a Lorentzian line shape at higher temperature, see Fig. 3b and d, that we attribute to lattice relaxation due to exciton-acoustic phonon coupling [13].…”
Section: The Neutral Exciton X 0 and The Trion X 1−mentioning
confidence: 81%
“…The interaction with optical phonons gives rise to satellites in the spectrum separated by multiples of the optical phonon frequency, which again are superimposed on a background due to the acoustic phonons. This type of spectra has been seen in many experimental and theoretical studies [50,78,51,62,67].…”
Section: Rabi Rotationsmentioning
confidence: 95%
“…3.1.3. Obviously, such a non-exponential and incomplete decay of the polarization, which in the spectral domain corresponds to strongly non-Lorentzian line shapes of the absorption or luminescence spectra [51,50,137], cannot be captured by a simple decay rate for the polarization. In fact, a naive calculation of phonon-induced relaxation rates according to Fermi's golden rule would give a zero result in this case, because the energies of the initial and final electronic state are the same and the phonon spectral density J(ω) is zero at ω = 0.…”
Section: Theoretical Methodsmentioning
confidence: 99%
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