2011
DOI: 10.1002/pssc.201001051
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Origin of the “green gap”: Increasing nonradiative recombination in indium‐rich GaInN/GaN quantum well structures

Abstract: Using time‐resolved photoluminescence spectroscopy on GaInN/GaN multiple quantum well structures, we analyze the radiative and nonradiative processes contributing to the “green gap” in GaN‐based light emitting devices. We observe that it is only partly caused by a reduced oscillator strength due to the Quantum Confined Stark Effect (QCSE) which becomes stronger with increasing indium concentration and well width. As the dominant effect we observe a reduction of nonradiative lifetimes when the indium concentrat… Show more

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Cited by 104 publications
(64 citation statements)
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“…For the 700°C InGaN growth, no emission was identified on the rough a-plane, possibly due to surface states introduced by roughening, acting as paths for nonradiative recombination 41 at high indium concentrations. 42 There were areas with emission peaks from the f10-10g facets at 2.35 eV, 2.62 eV, and a weak emission at 2.95 eV. This is probably caused by a varying indium fraction incorporation on the more irregular surfaces of this sample, while the 2.95 eV may originate from the first-grown region of the InGaN layer observable in the TEM image [see Fig.…”
Section: Characterization Of Indium Gallium Nitride Layersmentioning
confidence: 90%
“…For the 700°C InGaN growth, no emission was identified on the rough a-plane, possibly due to surface states introduced by roughening, acting as paths for nonradiative recombination 41 at high indium concentrations. 42 There were areas with emission peaks from the f10-10g facets at 2.35 eV, 2.62 eV, and a weak emission at 2.95 eV. This is probably caused by a varying indium fraction incorporation on the more irregular surfaces of this sample, while the 2.95 eV may originate from the first-grown region of the InGaN layer observable in the TEM image [see Fig.…”
Section: Characterization Of Indium Gallium Nitride Layersmentioning
confidence: 90%
“…67 and 68, while the A coefficient was assumed to be roughly proportional to N disl 69 (see also the recent studies on the impact of TDD on LED efficiency presented in Refs. 63,[70][71][72][73][74][75][76]. Auger coefficients were not forced to be the same in LDD and HDD LEDs because, although nominally identical, secondary ion mass spectrometry (SIMS) measures suggest that the QWs of the LDD devices have probably a smoother profile, which could imply a lower Auger rate.…”
Section: D Simulation Studymentioning
confidence: 99%
“…If the non-radiative recombination pathways are similar then it can be anticipated that the efficiency of green light emission would be less than that of blue emission. However, it has been reported 8,9 that this change in the radiative recombination lifetime is not sufficient to fully explain the reduction in efficiency. It has been suggested that there is also a reduction in the non-radiative recombination lifetime.…”
mentioning
confidence: 98%