2015
DOI: 10.1007/s11664-015-4132-7
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Nonradiative Recombination, Carrier Localization, and Emission Efficiency of AlGaN Epilayers with Different Al Content

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Cited by 6 publications
(3 citation statements)
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“…In the droop-effect, an increasing injection current leads to significant drop off in the emission efficiency of blue LEDs with indium gallium nitride (InGaN) MQW active layers [ 18 , 19 , 20 ]. The mechanisms of the efficiency droop in InGaN LEDs have been studied extensively, where carrier delocalization [ 21 , 22 , 23 ] and electron leakage [ 18 , 24 ] are proposed to be key reasons, while the most recent reports mainly pointing to Auger recombination as the main culprit [ 25 , 26 , 27 , 28 ]. Secondly, particularly in the modern high quantum efficiency LEDs, the efficiency droop limitations, current crowding and resistive loss become the most severe bottlenecks for high output power devices, confining their optimal high-efficiency performance at current densities well below 100 A/cm [ 29 , 30 , 31 , 32 , 33 , 34 ].…”
Section: Introductionmentioning
confidence: 99%
“…In the droop-effect, an increasing injection current leads to significant drop off in the emission efficiency of blue LEDs with indium gallium nitride (InGaN) MQW active layers [ 18 , 19 , 20 ]. The mechanisms of the efficiency droop in InGaN LEDs have been studied extensively, where carrier delocalization [ 21 , 22 , 23 ] and electron leakage [ 18 , 24 ] are proposed to be key reasons, while the most recent reports mainly pointing to Auger recombination as the main culprit [ 25 , 26 , 27 , 28 ]. Secondly, particularly in the modern high quantum efficiency LEDs, the efficiency droop limitations, current crowding and resistive loss become the most severe bottlenecks for high output power devices, confining their optimal high-efficiency performance at current densities well below 100 A/cm [ 29 , 30 , 31 , 32 , 33 , 34 ].…”
Section: Introductionmentioning
confidence: 99%
“…In the droop-effect an increasing injection current leads to significant drop off in the emission efficiency of blue LEDs with indium gallium nitride (InGaN) MQW active layers [18][19][20]. The mechanisms of the efficiency droop in InGaN LEDs have been studied extensively, where carrier delocalization [21][22][23] and electron leakage [18,24] are proposed to be key reasons, while the most recent reports mainly pointing to Auger recombination as the main culprit [25][26][27][28]. Secondly, particularly in the modern high quantum efficiency LEDs, the efficiency droop limitations, current crowding and resistive loss become the most severe bottlenecks for high output power devices, confining their optimal high-efficiency performance at current densities well below 100 A/cm 2 [29][30][31][32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…In addition, the AlGaN-based active region with wider bandgap has lower minority carrier diffusion length 31) in comparison with InGaN/GaN active regions due to heavier hole effective mass and fast recombination rate. 32) The reduced bulk minority carrier diffusion length suggests that carriers are less likely to reach sidewalls so that AlGaN material might be more tolerant of the surface nonradiative recombination caused by the sidewall damage. There are negligible differences in the peak wavelength and FWHM (full-width-at-halfmaximum) between LEDs with different mesa sizes, indicating no major difference in electrical fields within the active region or thermal effect.…”
mentioning
confidence: 99%