Abstract
By directly diagonalizing the many-body interacting Hamiltonian for two-model confinement potentials, we calculate the dipole-allowed optical-transition spectra for a few electrons confined in a small quantum dot subjected to a strong external magnetic field. We find substantial and qualitative many-body corrections to the optical-transition energies for quartic and flat-bottomed parabolic confinement in contrast to the well-studied purely parabolic confinement where optical transitions are known to be unaffected by interaction effects by virtue of the generalized Kohn’s theorem. We predict strong nonmonotonic structures as a function of the magnetic field in the magneto-optical excitation energy spectrum.
- Received 4 May 1993
DOI:https://doi.org/10.1103/PhysRevB.48.8454
©1993 American Physical Society