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Volumn 108, Issue 11, 2010, Pages

Effect of n-p-n heterostructures on interface recombination and semiconductor laser cooling

Author keywords

[No Author keywords available]

Indexed keywords

AUGER RECOMBINATION PROCESS; CARRIER DENSITY; COOLING CHARACTERISTICS; COOLING EFFICIENCY; DOPING CONCENTRATION; EXCITATION DENSITY; HETEROSTRUCTURES; INTERFACE RECOMBINATION; LUMINESCENCE DECAYS; MODEL ASSUMPTIONS; MODEL PARAMETERS; N-DOPING; N-P-N STRUCTURE; NON-RADIATIVE; NON-RADIATIVE LIFETIMES; NONRADIATIVE DECAYS; OPTICAL EXCITATIONS; PHOTOLUMINESCENCE CHARACTERISTICS; SEMICONDUCTOR HETEROSTRUCTURES; TEMPERATURE RANGE; TIME-DEPENDENT;

EID: 78751528328     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3517144     Document Type: Article
Times cited : (6)

References (24)
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  • 15
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    • a = 1014 cm-3, the electrons are the center minority carrier. As the p-doping is increased, the low density lifetime initially increases. Eventually, the center minority carrier becomes the holes, and then the low density lifetime decreases as the p-doping is increased
    • a = 1014 cm-3, the electrons are the center minority carrier. As the p-doping is increased, the low density lifetime initially increases. Eventually, the center minority carrier becomes the holes, and then the low density lifetime decreases as the p-doping is increased.
  • 17
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    • h (z) is very small. This results in almost no radiative recombination from these layers. Rather then calculate Beh and Bdh for GaInP, we ignore the tiny amount of radiative recombination that comes from the GaInP layers
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.