Abstract

The electronic structure, binding energy, and correlation functions of three different spatial configurations of ${\mathrm{D}}^{\mathrm{\ensuremath{-}}}$ centers in GaAs-based semiconductor structures are studied using a numerical technique that solves the two-electron Schr\"odinger equation for such systems. We compare our results for the quantum well ${\mathrm{D}}_{\mathrm{w}}^{\mathrm{\ensuremath{-}}}$ with experimental data and variational and diffusion Monte Carlo calculations. We demonstrate the existence of the spatially separated ${\mathrm{D}}_{\mathrm{s}}^{\mathrm{\ensuremath{-}}}$ center as a bound state, even in the regime of very low magnetic fields, and find interesting anticrossings among the energy levels in its electronic structure, which underlie a spectrum composition of a ${\mathrm{D}}^{0}$ donor center and a free electron in a magnetic field. For the remote ${\mathrm{D}}_{\mathrm{r}}^{\mathrm{\ensuremath{-}}}$ center we find that strong electron-electron correlations can give rise to magnetic-field-induced angular-momentum transitions, and as the magnetic field increases, these correlations weaken, while eventually the system magnetically evaporates approaching the classical unbound regime.

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