Quantum Ring Models and Action-Angle Variables; Journal of Computational and Theoretical Nanoscience; Vol. 40, iss. 22
| Parent link: | Journal of Computational and Theoretical Nanoscience: Scientific Journal Vol. 40, iss. 22.— 2011.— [P. 769-775] |
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| Další autoři: | , , , |
| Shrnutí: | Title screen We suggest to use the action-angle variables for the study of properties of (quasi)particles in quantum rings. For this purpose we present the action-angle variables for three two-dimensional singular oscillator systems. The first one is the usual (Euclidean) singular oscillator, which plays the role of the confinement potential for the quantum ring. We also propose two singular spherical oscillator models for the role of the confinement system for the spherical ring. The first one is based on the standard Higgs oscillator potential. We show that, in spite of the presence of a hidden symmetry, it is not convenient for the study of the system's behaviour in a magnetic field. The second model is based on the so-called CP1 oscillator potential and respects the inclusion of a constant magnetic field. Режим доступа: по договору с организацией-держателем ресурса |
| Jazyk: | angličtina |
| Vydáno: |
2011
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| Témata: | |
| On-line přístup: | http://dx.doi.org/10.1166/jctn.2011.1751 http://arxiv.org/abs/1008.3865 |
| Médium: | Elektronický zdroj Kapitola |
| KOHA link: | https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=641444 |
| Shrnutí: | Title screen We suggest to use the action-angle variables for the study of properties of (quasi)particles in quantum rings. For this purpose we present the action-angle variables for three two-dimensional singular oscillator systems. The first one is the usual (Euclidean) singular oscillator, which plays the role of the confinement potential for the quantum ring. We also propose two singular spherical oscillator models for the role of the confinement system for the spherical ring. The first one is based on the standard Higgs oscillator potential. We show that, in spite of the presence of a hidden symmetry, it is not convenient for the study of the system's behaviour in a magnetic field. The second model is based on the so-called CP1 oscillator potential and respects the inclusion of a constant magnetic field. Режим доступа: по договору с организацией-держателем ресурса |
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| DOI: | 10.1166/jctn.2011.1751 |