2018
DOI: 10.1016/j.infrared.2018.08.001
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Electroluminescence and photoluminescence of type-II InAs/InAsSb strained-layer superlattices in the mid-infrared

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Cited by 12 publications
(6 citation statements)
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“…show greater enhancement values (x10) compared with previous work 24,30 . The output power of the RCLED was measured to be 5.5 µW (external efficiency ≈ 0.024%) at 300 K rising to 45 µW at 77 K. We note that the electroluminescence of our RCLED lies entirely within the CO2 absorption band which coupled with the improved directionality provides a higher level of useful emission intensity compared with previous work 3,5,[13][14][15][16][17][18] .…”
Section: (D)mentioning
confidence: 58%
See 1 more Smart Citation
“…show greater enhancement values (x10) compared with previous work 24,30 . The output power of the RCLED was measured to be 5.5 µW (external efficiency ≈ 0.024%) at 300 K rising to 45 µW at 77 K. We note that the electroluminescence of our RCLED lies entirely within the CO2 absorption band which coupled with the improved directionality provides a higher level of useful emission intensity compared with previous work 3,5,[13][14][15][16][17][18] .…”
Section: (D)mentioning
confidence: 58%
“…Various LED structures have been developed for CO2 monitoring at 4.2 µm [9][10][11][12] , including bulk heterostructures of InAsSbP/InAsSb 13 , AlInSb 14 , InAsSb 15 , as well as InSb/InAs quantum dots 16 , InAs/InAsSb quantum wells and superlattices 3,5,17,18 . These devices typically exhibit 300 K output powers of a few microwatts, with an emittance of ~1-14 mW/cm -2 , but with broadband emission spectra resulting in low available power at the target wavelength.…”
mentioning
confidence: 99%
“…In our work, the main attention is paid to photoluminescent properties of a heterostructure based on bulk InAsSb compounds. The antimony-based materials were heavily studied in the past, but mostly in a form of lowdimensional structures [11][12][13], not in a bulk form. In this case, the novelty and importance of our work lies precisely in the disclosure of fundamental processes of radiative and non-radiative recombination in narrow-gap epitaxial layers based on antimonides.…”
Section: Introductionmentioning
confidence: 99%
“…Эти недостатки определяются фундаментальными причинами -спецификой зонной структуры рассматриваемых материалов и температурной зависимостью ширины запрещенной зоны E g полупроводников, и не могут быть преодолены в структурах на оcнове " объемных" материалов. Данные проблемы, однако, могут быть частично решены в структурах со сверхрешетками (СР), где возможно как подавление оже-рекомбинации [2,3], так и получение слабой температурной зависимости " оптической" E g (см., например, [4][5][6][7]). При этом СР предоставляют возможности для создания различных структур даже большие, чем твердые растворы.…”
Section: Introductionunclassified