Three-electron quantum dot in a magnetic field
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Three electrons confined by a parabolic well in a two-dimensional quantum dot and interacting via a logarithmic potential in a magnetic field are treated in the framework of the hyperspherical functions (HF) method by expanding the wave function in terms of the three-body symmetrized HF and the hyperradial functions of noninteracting trapped electrons. The binding energies and pair correlation function are calculated.
KeywordsPair Correlation Function Faddeev Equation Logarithmic Potential Homogeneous Algebraic Equation Classical Ground State
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