1994
DOI: 10.1103/physrevb.50.5189
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Theoretical investigation of the dynamic process of the illumination of GaAs

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Cited by 3 publications
(2 citation statements)
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“…We get good agreement with only one adjustable parameter, C 1 , determining the shape of the theoretical curve ͑C 2 is just a multiplicative factor͒. The value obtained from data fitting for C 1 =2ϫ 10 −17 s cm 3 is within an order of magnitude of the value computed from the literature, 16 3 ϫ 10 −18 s cm 3 . The present model predicts the peak just below the band gap as well as the dip at ϳ1.52 eV due to strong exciton absorption.…”
Section: Excitation and Recombination Modelsupporting
confidence: 79%
“…We get good agreement with only one adjustable parameter, C 1 , determining the shape of the theoretical curve ͑C 2 is just a multiplicative factor͒. The value obtained from data fitting for C 1 =2ϫ 10 −17 s cm 3 is within an order of magnitude of the value computed from the literature, 16 3 ϫ 10 −18 s cm 3 . The present model predicts the peak just below the band gap as well as the dip at ϳ1.52 eV due to strong exciton absorption.…”
Section: Excitation and Recombination Modelsupporting
confidence: 79%
“…The carrier lifetime is reduced for increasing temperatures, and therefore it is more difficult to detect them at the high temperature limit. The carrier lifetime is related to EL2 ͑or to EL2-like͒ density by ϭ͓C n (T)N t ͔ Ϫ1 , where C n (T) is the recombination rate of the free electrons in the conduction band to the EL2 ͑or to EL2-like͒ centers, 17 and N t is the defect concentration. At 150 K we have found for sample BH2 a carrier lifetime around 45 ps for this transition.…”
Section: Resultsmentioning
confidence: 99%