2011
DOI: 10.1016/j.jcrysgro.2010.10.031
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Improvement of structural and luminescence properties in InGaN/GaN multiple quantum wells by symmetrical thin low temperature-GaN layers

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Cited by 9 publications
(9 citation statements)
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“…8, a sharp and strong band edge emission is observed at 445 nm with a FWHM of 24.0 nm, indicating that high-quality GaN-based LED wafer is achieved on LSAT substrate using low-temperature RF-MBE working at high RF power which ensures the generation of high energetic N and hence the GaN nucleation at relatively low temperature. [47][48][49] From the PL peak location we can also deduce that the content of In in MQWs is about 0.13, which is consistent with our XRD measurement. 50 The EL measurement for the as-grown LED was also conducted at room temperature.…”
Section: Journal Of Materials Chemistry C Papersupporting
confidence: 86%
“…8, a sharp and strong band edge emission is observed at 445 nm with a FWHM of 24.0 nm, indicating that high-quality GaN-based LED wafer is achieved on LSAT substrate using low-temperature RF-MBE working at high RF power which ensures the generation of high energetic N and hence the GaN nucleation at relatively low temperature. [47][48][49] From the PL peak location we can also deduce that the content of In in MQWs is about 0.13, which is consistent with our XRD measurement. 50 The EL measurement for the as-grown LED was also conducted at room temperature.…”
Section: Journal Of Materials Chemistry C Papersupporting
confidence: 86%
“…The lower growth temperature of GaN QB can result in poor crystal quality of MQWs [ 12 , 13 ]. Moreover, in order to alleviate indium desorption or re-evaporation during the temperature ramp-up and GaN QB growth process, a thin low-temperature GaN cap layer (LT-cap) is usually deposited immediately after the growth of InGaN QW layer [ 14 17 ]. Nevertheless, the crystal quality of GaN LT-cap layer is very poor.…”
Section: Introductionmentioning
confidence: 99%
“…where ( ) is the PL intensity, 1 and 2 are the decay parameters, and and nr are the decay times for radiative and nonradiative recombination [17]. For the treated sample, the values of and nr were 6.2 × 10 −12 and 3.6 × 10 −9 s, respectively; for the untreated sample, they were 9.1 × 10 and 3.4 × 10 −9 s, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…Thus, the radiative decay time decreased as a result of pre-TMIn treatment, leading to a greater radiative recombination effect. Because carrier transport into weakly localized states requires a certain energy to overcome a potential barrier, it is more difficult for carriers to transfer into weakly localized states [17,18]. In the localized exciton model, trap centers are originated from a spatial disorder such as the fluctuation of indium within InGaN/GaN MQWs.…”
Section: Resultsmentioning
confidence: 99%