Study of the vertical transport in p-doped superlattices based on group III-V semiconductors

The electrical conductivity σ has been calculated for p -doped GaAs/Al 0.3 Ga 0.7 As and cubic GaN/Al 0.3 Ga 0.7 N thin superlattices (SLs). The calculations are done within a self-consistent approach to the k → ⋅ p → theory by means of a full six-band Luttinger-Kohn Hamiltonian, together with the P...

Full description

Saved in:
Bibliographic Details
Published in:Nanoscale research letters Vol. 6; no. 1; p. 175
Main Authors: dos Santos, Osmar FP, Rodrigues, Sara CP, Sipahi, Guilherme M, Scolfaro, Luísa MR, da Silva, Eronides F
Format: Journal Article
Language:English
Published: New York Springer New York 25-02-2011
BioMed Central Ltd
Springer
SpringerOpen
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:The electrical conductivity σ has been calculated for p -doped GaAs/Al 0.3 Ga 0.7 As and cubic GaN/Al 0.3 Ga 0.7 N thin superlattices (SLs). The calculations are done within a self-consistent approach to the k → ⋅ p → theory by means of a full six-band Luttinger-Kohn Hamiltonian, together with the Poisson equation in a plane wave representation, including exchange correlation effects within the local density approximation. It was also assumed that transport in the SL occurs through extended minibands states for each carrier, and the conductivity is calculated at zero temperature and in low-field ohmic limits by the quasi-chemical Boltzmann kinetic equation. It was shown that the particular minibands structure of the p -doped SLs leads to a plateau-like behavior in the conductivity as a function of the donor concentration and/or the Fermi level energy. In addition, it is shown that the Coulomb and exchange-correlation effects play an important role in these systems, since they determine the bending potential.
Bibliography:ObjectType-Article-1
SourceType-Scholarly Journals-1
ObjectType-Feature-2
content type line 23
ISSN:1556-276X
1931-7573
1556-276X
DOI:10.1186/1556-276X-6-175