2007
DOI: 10.1063/1.2745410
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Photoluminescence characteristics of InAs self-assembled quantum dots in InGaAs∕GaAs quantum well

Abstract: Three different InAs quantum dots ͑QDs͒ in an InGaAs/ GaAs quantum well were formed and investigated by time-resolved and temperature dependent photoluminescence ͑PL͒. A strong PL signal emitting at ϳ1.3 m can be obtained at room temperature with a full width at half maximum of only 28 meV. Dots-in-a-well structures result in strong stress release and large size InAs QDs which lead to narrowing and redshifting of PL emissions, enhancement of carrier migration, increasing carrier density in QDs, achievement of … Show more

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Cited by 15 publications
(11 citation statements)
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“…(iii) High-T range (220-300 K), where the observed decrease of s d is attributed to thermionic losses. 28 The observed increase in s d in the mid-T range is characterized by an activation energy between 20 and 80 meV, as 194306 (2013) in other similar nanostructures, 41,42 InAs/GaAs selfassembled QDs 43,44 and quantum ring nanostructures. 45,46 The origin of this behavior has been attributed to a thermally induced population of dark excitons; 44,45 where transitions p e -s e (or p h -s h ), initially forbidden, becomes allowed due to thermal transfer.…”
Section: -2mentioning
confidence: 77%
“…(iii) High-T range (220-300 K), where the observed decrease of s d is attributed to thermionic losses. 28 The observed increase in s d in the mid-T range is characterized by an activation energy between 20 and 80 meV, as 194306 (2013) in other similar nanostructures, 41,42 InAs/GaAs selfassembled QDs 43,44 and quantum ring nanostructures. 45,46 The origin of this behavior has been attributed to a thermally induced population of dark excitons; 44,45 where transitions p e -s e (or p h -s h ), initially forbidden, becomes allowed due to thermal transfer.…”
Section: -2mentioning
confidence: 77%
“…Besides, at higher temperature ( T > T c ), there is a faster reduction in the average PL lifetime due to the dominance of non‐radiative recombination. There are several competing mechanisms which are responsible for such kind of phenomena such as; (i) thermally induced carrier distribution among the QDs, (ii) thermally induced population of dark excitons, and (iii) non‐radiative recombination …”
Section: Resultsmentioning
confidence: 99%
“…On the other hand, a full-width at half-maximum (FWHM) of the InAs QDs at temperature ranging from 15 to 180 K was maintained about 40 meV. As increase the temperature above 180 K, the FWHM drastically increased with temperature due to the effect of electron-phonon scattering and thermal broadening [14]. It was considered that the fast red-shift of ground-state PL peak position and the increase of FHWM at the temperature above 180 K may be resulted from an increase in the migration rate from the small QDs with higher energy level to larger QDs with lower energy level [15].…”
Section: Resultsmentioning
confidence: 99%