DC Field | Value | Language |
dc.contributor.author | Baran, A. V. | - |
dc.contributor.author | Kudryashov, V. V. | - |
dc.date.accessioned | 2022-02-02T06:09:39Z | - |
dc.date.available | 2022-02-02T06:09:39Z | - |
dc.date.issued | 2021 | - |
dc.identifier.citation | Baran, A. V. Energy levels of an electron in a circular quantum dot in the presence of spin-orbit interactions / Baran A. V., Kudryashov V. V. // Доклады БГУИР. – 2021. – № 19(8). – С. 20–25. – DOI : https://doi.org/10.35596/1729-7648-2021-19-8-20-25. | ru_RU |
dc.identifier.uri | https://libeldoc.bsuir.by/handle/123456789/46635 | - |
dc.description.abstract | The two-dimensional circular quantum dot in a double semiconductor heterostructure is simulated by
a new axially symmetric smooth potential of finite depth and width. The presence of additional potential
parameters in this model allows us to describe the individual properties of different kinds of quantum dots.
The influence of the Rashba and Dresselhaus spin-orbit interactions on electron states in quantum dot is
investigated. The total Hamiltonian of the problem is written as a sum of unperturbed part and perturbation.
First, the exact solution of the unperturbed Schrödinger equation was constructed. Each energy level of the
unperturbed Hamiltonian was doubly degenerated. Further, the analytical approximate expression for energy
splitting was obtained within the framework of perturbation theory, when the strengths of two spin-orbit
interactions are close. The numerical results show the dependence of energy levels on potential parameters. | ru_RU |
dc.language.iso | en | ru_RU |
dc.publisher | БГУИР | ru_RU |
dc.subject | доклады БГУИР | ru_RU |
dc.subject | circular quantum dots | ru_RU |
dc.subject | confinement potential | ru_RU |
dc.subject | spin-orbit interactions | ru_RU |
dc.subject | energy levels | ru_RU |
dc.title | Energy levels of an electron in a circular quantum dot in the presence of spin-orbit interactions | ru_RU |
dc.type | Статья | ru_RU |
Appears in Collections: | № 19(8)
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