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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Sears, K.
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Topics
Publications (7/7 displayed)
- 2010Electrical properties of Si-XII and Si-III formed by nanoindentationcitations
- 2007Modeling and characterization of InAsGaAs quantum dot lasers grown using metal organic chemical vapor depositioncitations
- 2006A transmission electron microscopy study of defects formed through the capping layer of self-assembled InAs/GaAs quantum dot samplescitations
- 2006Quantum Dots and Nanowires Grown by Metal-Organic Chemical Vapor Deposition for Optoelectronic Device Applicationscitations
- 2006The role of arsine in the self-assembled growth of InAs/GaAs quantum dots by metal organic chemical vapor depositioncitations
- 2005InAs quantum dots grown on InGaAs buffer layers by metal-organic chemical vapor depositioncitations
- 2005In0.5 Ga0.5As/GaAs quantum dot infrared photodetectors grown by metal-organic chemical vapor depositioncitations
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article
Modeling and characterization of InAsGaAs quantum dot lasers grown using metal organic chemical vapor deposition
Abstract
<p>We report on the lasing characteristics of three- and five-stack InAsGaAs quantum dot (QD) lasers grown by metal organic chemical vapor deposition. By increasing the number of stacked dot layers to 5, lasing was achieved from the ground state at 1135 nm for device lengths as short as 1.5 mm (no reflectivity coatings). The unamplified spontaneous emission and Z ratio as a function of injection current were also investigated. While the five-stack QD lasers behaved as expected with Z ratios of ≈2 prior to lasing, the three-stack QD lasers, which lased from the excited state, exhibited Z -ratio values as high as 4. A simple model was developed and indicated that high Z ratios can be generated by three nonradiative recombination pathways: (i) high monomolecular recombination within the wetting layer, (ii) Auger recombination involving carriers within the QDs ("unmixed" Auger), and (iii) Auger recombination involving both the QD and wetting layer states ("mixed" Auger), which dominate once the excited and wetting layer states become populated.</p>