Application of type II W-quantum-well diode lasers for high-dynamic-temperature-range infrared scene projection

2008 ◽  
Vol 47 (8) ◽  
pp. 086401 ◽  
Author(s):  
Gary Ballard
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.


1998 ◽  
Vol 108 (4) ◽  
pp. 205-209 ◽  
Author(s):  
J Haetty ◽  
E.H Lee ◽  
H Luo ◽  
A Petrou ◽  
J Warnock

1998 ◽  
Vol 32 (6) ◽  
pp. 665-667
Author(s):  
V. V. Bondarenko ◽  
V. V. Zabudskii ◽  
F. F. Sizov

1965 ◽  
Vol 180 (1) ◽  
pp. 285-294 ◽  
Author(s):  
F. U. Mahtab ◽  
W. Johnson ◽  
R. A. C. Slater

The dynamic indentation of copper (B.S. 1433) and an aluminium alloy (B.S. 1476 HE 10) has been investigated, using cylindro-conical projectiles fired from an air-actuated gun. The experiments were performed with impact velocities varying between 1000 and 2500 in/s and at elevated temperatures up to 600°C for the copper and 550°C for the aluminium alloy. The magnitude of the corresponding range of mean strain rate was then 103-104/s, depending upon the material; impact velocity and temperature (see Appendix I). For the range of impact velocities investigated no consequential transition temperature † was encountered. The dynamic temperature coefficient† thus remained constant throughout the test temperature range for each material. This dynamic temperature coefficient was found to be equal to the static temperature coefficient corresponding to the sub-transitional temperature range for the respective materials. The mean effective dynamic indentation pressure is shown to decrease with temperature but the ratio of this dynamic pressure to the static indentation pressure increases with temperature. Strain rate effects for both materials were negligible for sub-transitional temperatures but become important at super-transitional temperatures. It was observed that the parameters on which the strain rate effect depends are in some way related to the absolute melting point of a pure metal.


2003 ◽  
Vol 83 (14) ◽  
pp. 2742-2744 ◽  
Author(s):  
I. Vurgaftman ◽  
J. R. Meyer ◽  
N. Tansu ◽  
L. J. Mawst

1994 ◽  
Vol 50 (8) ◽  
pp. 5787-5790 ◽  
Author(s):  
J. Ding ◽  
M. Hagerott ◽  
P. Kelkar ◽  
A. V. Nurmikko ◽  
D. C. Grillo ◽  
...  

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