TY - JOUR
T1 - A generalized plane-wave formulation of k · p formalism and continuum-elasticity approach to elastic and electronic properties of semiconductor nanostructures
AU - Marquardt, Oliver
AU - Boeck, Sixten
AU - Freysoldt, Christoph
AU - Hickel, Tilmann
AU - Schulz, Stefan
AU - Neugebauer, Jörg
AU - O'Reilly, Eoin P.
PY - 2014/12
Y1 - 2014/12
N2 - We present a generalized and flexible plane-wave based implementation of the multiband k·p formalism to study the electronic properties of semiconductor nanostructures. All ingredients of the modeling process, namely the Hamiltonian, the nanostructure's geometry and the required material parameters, are defined in human-readable input files that can be easily generated and modified. The generalized k·p model can contain an arbitrary number of directly treated bands as well as strain, piezoelectric, and external potentials. All calculations can be performed for arbitrary crystal structures. The nanostructure is described in terms of a real-space composition map that may contain an arbitrary number of base compounds and alloys. We demonstrate the applicability and flexibility of our implementation for the example of (111)-oriented, site-controlled InGaAs quantum dots, where a rotated eight-band k·p Hamiltonian is employed. As a second example, a 14-band k·p model that captures the bulk inversion asymmetry of the zinc-blende lattice is applied for the case of a pyramidal (0 0 1)-oriented InAs/GaAs quantum dot. Here we show that the explicit treatment of 14 bands removes the well known shortcoming of eight-band k·p models for (0 0 1)-oriented zinc-blende quantum dots which leads to artificially degenerate p-like electron states.
AB - We present a generalized and flexible plane-wave based implementation of the multiband k·p formalism to study the electronic properties of semiconductor nanostructures. All ingredients of the modeling process, namely the Hamiltonian, the nanostructure's geometry and the required material parameters, are defined in human-readable input files that can be easily generated and modified. The generalized k·p model can contain an arbitrary number of directly treated bands as well as strain, piezoelectric, and external potentials. All calculations can be performed for arbitrary crystal structures. The nanostructure is described in terms of a real-space composition map that may contain an arbitrary number of base compounds and alloys. We demonstrate the applicability and flexibility of our implementation for the example of (111)-oriented, site-controlled InGaAs quantum dots, where a rotated eight-band k·p Hamiltonian is employed. As a second example, a 14-band k·p model that captures the bulk inversion asymmetry of the zinc-blende lattice is applied for the case of a pyramidal (0 0 1)-oriented InAs/GaAs quantum dot. Here we show that the explicit treatment of 14 bands removes the well known shortcoming of eight-band k·p models for (0 0 1)-oriented zinc-blende quantum dots which leads to artificially degenerate p-like electron states.
KW - Continuum-elasticity theory
KW - Electronic structure
KW - k · p Formalism
KW - Nanostructures
KW - Plane wave
UR - https://www.scopus.com/pages/publications/84906537740
U2 - 10.1016/j.commatsci.2014.06.047
DO - 10.1016/j.commatsci.2014.06.047
M3 - Article
AN - SCOPUS:84906537740
SN - 0927-0256
VL - 95
SP - 280
EP - 287
JO - Computational Materials Science
JF - Computational Materials Science
ER -