2007
DOI: 10.1088/0957-4484/18/35/355401
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Relaxation-induced lattice misfits and their effects on the emission properties of InAs quantum dots

Abstract: Strain relaxation in InAs/InGaAs quantum dots (QDs) is shown to introduce misfits in the QD and neighboring GaAs bottom layer. A capacitance-voltage profiling shows an electron accumulation peak at the QD with a long emission time, followed by additional carrier depletion caused by the misfits in the GaAs bottom layer. The emission-time increase is explained by the suppression of tunneling for the QD excited states due to the additional carrier depletion. As a result, electrons are thermally activated from the… Show more

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Cited by 10 publications
(18 citation statements)
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“…[1] In addition, the strain relaxation induces a misfit defect at the bottom of the InAs QDs. This defect has been confirmed by transmission electron microscopy (TEM) images [2,3]. The misfit defect also enhances the confinement of the QDs.…”
Section: Sample Fabrication and Propertiesmentioning
confidence: 69%
“…[1] In addition, the strain relaxation induces a misfit defect at the bottom of the InAs QDs. This defect has been confirmed by transmission electron microscopy (TEM) images [2,3]. The misfit defect also enhances the confinement of the QDs.…”
Section: Sample Fabrication and Propertiesmentioning
confidence: 69%
“…This emission time is very short, as indicated by 'InAs QDs' in figure 3. The Ninduced defect state (indicated by a dashed line) can suppress the tunneling emission, presumably by inducing additional carrier depletion [11] and increasing the tunneling width (the detailed band structure is not shown). Electrons escaping out of the GS have to emit to a state near the GaAs CB, leading to a significant emission energy increase from 0.058 to 0.15 eV and several orders of magnitude increase in the emission time.…”
Section: Resultsmentioning
confidence: 99%
“…This defect state is associated with relaxationinduced lattice misfits observed by Fourier transformed cross-sectional TEM. 25 Annealing at 650°C does not much affect the concentration and emission parameters of this defect state. We had investigated the DLTS spectra by varying filling pulse duration time and found that the amplitude of the defect state saturated when filling pulse duration time was increased to about 1 ms.…”
Section: A Electron Distribution In the Qdsmentioning
confidence: 91%