K. L. Janssens
University of Antwerp
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Featured researches published by K. L. Janssens.
Journal of Applied Physics | 2002
M. Tadić; F. M. Peeters; K. L. Janssens; Marek Korkusinski; Pawel Hawrylak
A comparative study is made of the strain distribution in cylindrical InAs/GaAs and InP/InGaP self-assembled quantum dots as obtained from isotropic elasticity theory, the anisotropic continuum mechanical model, and from atomistic calculations. For the isotropic case, the recently proposed approach [J. H. Davies, J. Appl. Phys. 84, 1358 (1998)] is used, while the finite-element method, the valence force field method, and Stillinger–Weber potentials are employed to calculate the strain in anisotropic structures. We found that all four methods result in strain distributions of similar shapes, but with notable quantitative differences inside the dot and near the disk–matrix boundary. The variations of the diagonal strains with the height of the quantum dot, with fixed radius, as calculated from all models, are almost linear. Furthermore, the energies of the band edges in the two types of quantum dots are extracted from the multiband effective-mass theory by inserting the strain distributions as obtained by t...
Physical Review B | 2002
K. L. Janssens; B. Partoens; F. M. Peeters
We theoretically studied the Stark effect on an exciton in single and vertically coupled type-I and type-II quantum dots. Only for the single type-I dot does the exciton energy show a parabolic dependence on the applied field. A dipole moment is induced by the applied electric field for vertically coupled type-I dots and for type-II dots, leading to a linear dependence of the Stark shift on the electric field. Furthermore, we predict that spontaneous symmetry breaking can occur for vertically coupled type-II dots leading to a permanent dipole moment.
Physical Review B | 2002
K. L. Janssens; B. Partoens; F. M. Peeters
The properties of an exciton in a type-II quantum dot are studied under the influence of a perpendicular applied magnetic field. The dot is modeled by a quantum disk with radius R, thickness d and the electron is confined in the disk, whereas the hole is located in the barrier. The exciton energy and wave functions are calculated applying a self-consistent mean-field theory in the Hartree approximation using a finite difference mesh method. We distinguish two different regimes, namely,
Physica E-low-dimensional Systems & Nanostructures | 2002
M. Tadić; F. M. Peeters; B. Partoens; K. L. Janssens
d\ensuremath{\ll}2R
Archive | 2004
F. M. Peeters; M. Tadić; K. L. Janssens; B. Partoens
(the hole is located above and below the disk) and
Recent trends on physical phenomena in high magnetic fields / Vagener, I.D. [edit.] | 2003
F. M. Peeters; K. L. Janssens; B. Partoens
d\ensuremath{\gg}2R
Physica Status Solidi (a) | 2002
K. L. Janssens; B. Partoens; F. M. Peeters
(the hole is located at the radial boundary of the disk), for which angular momentum (l) transitions are predicted with increasing magnetic field. We also considered a system of two vertically coupled dots where now an extra parameter is introduced, namely, the interdot distance
Physical Review B | 2002
M. Tadić; F. M. Peeters; K. L. Janssens
{d}_{z}.
Physical Review B | 2001
K. L. Janssens; B. Partoens; F. M. Peeters
For a sufficient large magnetic field, each
Physical Review B | 2003
K. L. Janssens; B. Partoens; F. M. Peeters
{l}_{h}