Quantum-Mechanical generalization of the Thomas–Fermi model
- Authors: Chaplik A.V.1
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Affiliations:
- Rzhanov Institute of Semiconductor Physics
- Issue: Vol 105, No 9 (2017)
- Pages: 601-605
- Section: Methods of Theoretical Physics
- URL: https://journals.rcsi.science/0021-3640/article/view/160293
- DOI: https://doi.org/10.1134/S0021364017090089
- ID: 160293
Cite item
Abstract
The interaction between particles in the mean-field approximation of the many-body theory is often taken into account with the use of the semiclassical description of the particle motion. However, quantization of a part of the degrees of freedom becomes essential in certain cases. In this work, two such cases where nonlinear wave equations appear have been considered: electrons in a quantum well and excitons in a trap. In the case of indirect excitons in an annular trap, the one-dimensional Gross–Pitaevskii equation permits an analytical solution and it turns out that there can be no bound state in a one-dimensional symmetric potential well. This makes the problem qualitatively different from a similar one-body problem. In the case of electrons in a quantum well, the nonlinear integro-differential equation does not have an exact solution and the allowed energy levels have been found by the direct variational method.
About the authors
A. V. Chaplik
Rzhanov Institute of Semiconductor Physics
Author for correspondence.
Email: chaplik@isp.nsc.ru
Russian Federation, Novosibirsk, 630090
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