TheE1–E2 center in gallium arsenide is the divacancy

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The E1-E2 center in gallium arsenide is the divacancy.

Based on defect energy levels computed from first-principles calculations, it is shown the E1-E2 center in irradiated GaAs cannot be due to an isolated arsenic vacancy. The only simple intrinsic defect with levels compatible with E1 and E2 is the divacancy. The arsenic monovacancy is reassigned to the E3 center in irradiated GaAs. These new assignments are shown to reconcile a number of seeming...

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Although photoluminescence from gallium-arsenide (GaAs) deep-centers was first observed in the 1960s, semiconductor lasers have always utilized conduction-to-valence-band transitions. Here we review recent materials studies leading to the first GaAs deep-center laser. First, we summarize well-known properties: nature of deep-center complexes, Franck-Condon effect, photoluminescence. Second, we ...

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GALLIUM ARSENIDE 1. Exposure Data

1.1.3 Chemical and physical properties of the pure substance (a) Description: Grey, cubic crystals (Lide, 2003) (b) Melting-point: 1238 °C (Lide, 2003) (c) Density: 5.3176 g/cm (Lide, 2003) (d) Solubility: Insoluble in water (Wafer Technology Ltd, 1997); slightly soluble in 0.1 M phosphate buffer at pH 7.4 (Webb et al., 1984) (e) Stability: Decomposes with evolution of arsenic vapour at tempera...

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GALLIUM ARSENIDE 1. Exposure Data

1.1.3 Chemical and physical properties of the pure substance (a) Description: Grey, cubic crystals (Lide, 2003) (b) Melting-point: 1238 °C (Lide, 2003) (c) Density: 5.3176 g/cm (Lide, 2003) (d) Solubility: Insoluble in water (Wafer Technology Ltd, 1997); slightly soluble in 0.1 M phosphate buffer at pH 7.4 (Webb et al., 1984) (e) Stability: Decomposes with evolution of arsenic vapour at tempera...

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ژورنال

عنوان ژورنال: Journal of Physics: Condensed Matter

سال: 2015

ISSN: 0953-8984,1361-648X

DOI: 10.1088/0953-8984/27/7/075801