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Electrical Activity of Extended Defects in Relaxed In <sub>x</sub> Ga <sub>1−x</sub> As Hetero-Epitaxial Layers

Cor ClaeysDepartment of Electrical Engineering, KU Leuven, B-3001 Leuven, BelgiumPo-Chun HsuImec, B-3001 Leuven, BelgiumY. MolsImec, B-3001 Leuven, BelgiumHyunjin HanImec, B-3001 Leuven, BelgiumH. BenderImec, B-3001 Leuven, BelgiumF. C. SeidelImec, B-3001 Leuven, BelgiumPatrick CarolanImec, B-3001 Leuven, BelgiumClément MercklingImec, B-3001 Leuven, BelgiumA. AlianImec, B-3001 Leuven, BelgiumNiamh WaldronImec, B-3001 Leuven, BelgiumGeert EnemanImec, B-3001 Leuven, BelgiumNadine CollaertImec, B-3001 Leuven, BelgiumMarc HeynsImec, B-3001 Leuven, BelgiumE. SimoenGhent University, Department Solid State Sciences, 9000 Gent, Belgium
2020en
ABI

Аннотация

The electrical activity of extended defects in III–V materials, combining different analysis methods based on lifetime extraction from diode current-voltage characteristics, time resolved photoluminescence (TRPL) and deep level studies using Deep Level Transient Spectroscopy (DLTS) is reviewed. To that purpose p + n junction diodes have been fabricated in In 0.53 Ga 0.47 As hetero-epitaxial layers on semi-insulating InP or GaAs substrates. By depositing a strained buffer layer, the Extended Defect Density (EDD) can be varied over several decades, enabling a systematic study of their electrical impact in the same range. The defect densities are determined by High-Resolution X-ray Diffraction (HR-XRD), DLTS and Electron Channeling Contrast (ECCI) techniques. The generation and recombination (GR) lifetimes of the In 0.53 Ga 0.47 As layers become dominated by the EDs for densities above about 3 × 10 7 cm −2 , whereby the dominant GR level moves closer to the mid gap position. This is supported by DLTS investigations, showing the occurrence of specific electron traps for defective epi layers, which exhibit a capture behavior that is typical for extended defects.

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