Intervalley scattering of electrons by short-wave phonons in (GaAs) sub(8)(AlAs) sub(8)(001) superlattice

Intervalley transitions induced by short-wavelength phonons in the conduction band of a superlattice (GaAs) sub(8)(AlAs) sub(8)(001) are investigated on the basis of the pseudopotential method and in the phenomenological model of interatomic forces. The main attention in the study centers around the...

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Bibliographic Details
Published in:Superlattices and microstructures 2016-05, Vol.93, p.280-289
Main Authors: Grinyaeva, S N, Nikitinaa, L N, Tyuterevb, V G
Format: Article
Language:English
Subjects:
Conduction band
Phonons
Pseudopotentials
Sphalerite
Superlattices
Valleys
Vibration
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Summary:Intervalley transitions induced by short-wavelength phonons in the conduction band of a superlattice (GaAs) sub(8)(AlAs) sub(8)(001) are investigated on the basis of the pseudopotential method and in the phenomenological model of interatomic forces. The main attention in the study centers around the transitions associated with the vibrations confined inside the layers. It is shown that the deformation potentials for the majority of intervalley transitions in a superlattice exceed the potentials of corresponding transitions in the binary crystals because of the localization of atomic displacements and wavefunctions of electrons inside the same layer of the superlattice. The bottom of the conduction band in (GaAs) sub(8)(AlAs) sub(8)(001) superlattice corresponds to the states View the MathML source Gamma 1(1), Z sub(3), M sub(1), M sub(4) originating from sphalerite's View the MathML source X[macr] valleys localized in AlAs layers. Transitions between them are the most intense ones and they are caused by optical vibrations of Al atoms. "Semi-interface" vibrations being mainly localized in the one side of the GaAs layer are involved in the View the MathML source Gamma 1(2)-X1, View the MathML source Gamma 1(2)-R1 and X sub(1)-Z sub(1) transitions which are analogs of View the MathML source Gamma [macr]-L[macr] transitions in binaries. The transitions View the MathML source Gamma 1(2)-M1 and View the MathML source Gamma 1(2)-M4 are governed by smooth parts of wave-functions and pseudopotentials. As a consequence their intensities are comparable with those of View the MathML source Gamma [macr]-X[macr] sphalerite transitions in spite that these states are localized in the different layers of the superlattice.
ISSN:0749-6036
DOI:10.1016/j.spmi.2016.03.008