2021
DOI: 10.1016/j.jlumin.2021.118393
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Influence of the doping type on the temperature dependencies of the photoluminescence efficiency of InGaAlAs/InGaAs/InP heterostructures

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Cited by 4 publications
(3 citation statements)
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“…Full width at half maximum (FWHM) of the MQW PL band is 12−18 meV at the nitrogen temperature when FWHM is defined mainly by fluctuations of the well composition and thickness rather than by the temperature expansion. The measured PL band width is typical of the InGaAlAs/InAlAs MQW [14,15] and is relevant to the composition fluctuations within 1−2%.…”
mentioning
confidence: 88%
“…Full width at half maximum (FWHM) of the MQW PL band is 12−18 meV at the nitrogen temperature when FWHM is defined mainly by fluctuations of the well composition and thickness rather than by the temperature expansion. The measured PL band width is typical of the InGaAlAs/InAlAs MQW [14,15] and is relevant to the composition fluctuations within 1−2%.…”
mentioning
confidence: 88%
“…Квантовые точки (КТ) используются в качестве активных областей для широкого круга лазерных применений [1], в том числе в лазерах с микрорезонатором для нейроморфных вычислений [2,3]. В источниках одиночных фотонов требуется малая плотность КТ [4], однако в лазерных структурах с вертикальным микрорезонатором, где изначально объем активной области минимален, наоборот, требуется повышать плотность КТ, чтобы достигнуть порога лазерной генерации. Оптическое усиление активных областей на основе " идеальных" КТ должно превышать оптическое усиление активных областей на основе квантовых ям (КЯ), однако на практике ситуация иная, что обусловлено эффектом неоднородного уширения в ансамбле КТ.…”
Section: Introductionunclassified
“…Quantum dots (QDs) are used as active regions for a wide range of laser applications [1], including in lasers with a microresonator for neuromorphic computing [2,3]. In single photon sources, a low QD density is required [4], however, in laser structures with a vertical microresonator, where initially the volume of the active region is minimal, on the contrary, it is necessary to increase the QD density in order to reach the laser generation threshold. The optical gain of the active regions based on " ideal" QD should exceed the optical gain of the active regions based on quantum wells, but in practice the situation is different, due to the effect of inhomogeneous broadening in the ensemble of QDs.…”
Section: Introductionmentioning
confidence: 99%