2002
DOI: 10.1063/1.1459622
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Disorder-induced photoluminescence up-conversion in InAs/GaAs quantum-dot samples

Abstract: Photoluminescence up-conversion under cw excitation in semiconductor quantum-dot structures is systematically studied in a sample exhibiting a crossover between two-dimensional and three-dimensional (3D) growth modes. We probe the existence of carrier up-conversion by using ultrathin quantum wells close to the quantum-dot layer. We show that the efficiency of the up-conversion is closely related to the disorder induced by the 3D-growth mode of the quantum dots.

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Cited by 12 publications
(15 citation statements)
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“…2(b)]. As has been discussed in previous reports, [6][7][8] this absorption tail is attributed to the continuous states between the WL and QDs. 500 nm 14 nm Fig.…”
Section: Methodssupporting
confidence: 49%
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“…2(b)]. As has been discussed in previous reports, [6][7][8] this absorption tail is attributed to the continuous states between the WL and QDs. 500 nm 14 nm Fig.…”
Section: Methodssupporting
confidence: 49%
“…2(b)]. [6][7][8] The integrated PL intensity is constant or rather increases in this temperature range, indicating the absence of nonradiative recombination centers in the channels and a higher PL efficiency (longer radiative lifetime 23) ) of the low-energy QDs preferentially occupied during the carrier redistribution. The detailed analysis of the temperature-dependent PL peak position and width in this temperature range provides important insight into the properties of these channels.…”
Section: Resultsmentioning
confidence: 99%
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“…Let us now discuss the power dependence introduced for γ 1 and γ 2 . Considering the evolution of the barrier electron (hole) population N e (N h ) under a non-resonant excitation [37] and the fact that the photoluminescence of the GaAs barrier is not influenced by the QDs population [38], the populations N e and N h created by the optical gate are governed by bimolecular interband radiative recombination [13,37] and are proportional to √ P gate . The carriers can be then captured in the QD and the defect in its vicinity, either by the emission of optical phonons, or by Auger processes.…”
Section: Theory Versus Experimental Resultsmentioning
confidence: 99%