Magnetic-field-induced binding of few-electron systems in shallow quantum dots
arXiv:cond-mat/0606514 · doi:10.1103/PhysRevB.74.115310
Abstract
Binding of few-electron systems in two-dimensional potential cavities in the presence of an external magnetic field is studied with the exact diagonalization approach. We demonstrate that for shallow cavities the few-electron system becomes bound only under the application of a strong magnetic field. The critical value of the depth of the cavity allowing the formation of a bound state decreases with magnetic field in a non-smooth fashion, due to the increasing angular momentum of the first bound state. In the high magnetic field limit the binding energies and the critical values for the depth of the potential cavity allowing the formation of a bound system tend to the classical values.
References in corpus (10)
- The microscopic nature of localization in the quantum Hall effect
- Few-electron eigenstates of concentric double quantum rings
- Trial wave functions with long-range Coulomb correlations for two-dimensional N-electron systems in high magnetic fields
- Off center centers in a quantum well in the presence of a perpendicular magnetic field: angular momentum transition and magnetic evaporation
- Electron spin and charge switching in a coupled quantum dot quantum ring system
- The Addition Spectrum and Koopmans' Theorem for Disordered Quantum Dots
- Impurity effects in few-electron quantum dots: Incipient Wigner molecule regime
- Interactions and Disorder in Quantum Dots: Instabilities and Phase Transitions
- Accuracy of the Hartree-Fock method for Wigner molecules at high magnetic fields
- Disorder and interaction induced pairing in the addition spectra of quantum dots