InGaN∕GaN Multiple-Quantum-Well LEDs with Si-Doped Barriers

2008 ◽  
Vol 155 (6) ◽  
pp. H455 ◽  
Author(s):  
H. Hung ◽  
K. T. Lam ◽  
S. J. Chang ◽  
C. H. Chen ◽  
H. Kuan ◽  
...  
2009 ◽  
Vol 9 (5) ◽  
pp. 943-945 ◽  
Author(s):  
Soon Il Jung ◽  
Ilgu Yun ◽  
Chang Myung Lee ◽  
Joo In Lee

2016 ◽  
Vol 119 (5) ◽  
pp. 055708 ◽  
Author(s):  
M. J. Davies ◽  
S. Hammersley ◽  
F. C.-P. Massabuau ◽  
P. Dawson ◽  
R. A. Oliver ◽  
...  

2002 ◽  
Vol 744 ◽  
Author(s):  
J. C. Shin ◽  
W. J. Choi ◽  
I. K. Han ◽  
Y. J. Park ◽  
J. I. Lee ◽  
...  

ABSTRACTWe have studied the change of the spectral response in a quantum well infrared photodetector (QWIP) by using the impurity-free vacancy disordering (IFVD) to change the bandgap of the GaAs/AlGaAs multiple quantum well absorption layer. IFVD process has been carried out with PECVD-grown SiO2 capping on the MOCVD-grown QWIP structure, whose absorption region consists of 25 periods of 3.6nm thick Si-doped GaAs well and 50nm thick Al0.24Ga0.76As barrier. The PL peak of MQW decreased with the increase of annealing temperature and time from 802 nm to 700 nm at 15 K. The fabricated QWIP whose absorption region was intermixed at 850 °C by IFVD technique showed the maximum change in spectral response from 8 to 10 um when compared to a QWIP without intermixing. This result implies that the intermixing technology can be used to make multicolor QWIP without growing multiple IR absorption regions.


1987 ◽  
Vol 48 (C5) ◽  
pp. C5-457-C5-461
Author(s):  
C. J. SUMMERS ◽  
K. F. BRENNAN ◽  
A. TORABI ◽  
H. M. HARRIS ◽  
J. COMAS

2003 ◽  
Vol 764 ◽  
Author(s):  
X. A. Cao ◽  
S. F. LeBoeuf ◽  
J. L. Garrett ◽  
A. Ebong ◽  
L. B. Rowland ◽  
...  

Absract:Temperature-dependent electroluminescence (EL) of InGaN/GaN multiple-quantum-well light-emitting diodes (LEDs) with peak emission energies ranging from 2.3 eV (green) to 3.3 eV (UV) has been studied over a wide temperature range (5-300 K). As the temperature is decreased from 300 K to 150 K, the EL intensity increases in all devices due to reduced nonradiative recombination and improved carrier confinement. However, LED operation at lower temperatures (150-5 K) is a strong function of In ratio in the active layer. For the green LEDs, emission intensity increases monotonically in the whole temperature range, while for the blue and UV LEDs, a remarkable decrease of the light output was observed, accompanied by a large redshift of the peak energy. The discrepancy can be attributed to various amounts of localization states caused by In composition fluctuation in the QW active regions. Based on a rate equation analysis, we find that the densities of the localized states in the green LEDs are more than two orders of magnitude higher than that in the UV LED. The large number of localized states in the green LEDs are crucial to maintain high-efficiency carrier capture at low temperatures.


2000 ◽  
Author(s):  
William J. Siskaninetz ◽  
Hank D. Jackson ◽  
James E. Ehret ◽  
Jeffrey C. Wiemeri ◽  
John P. Loehr

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