Effect of magnetic field on resonant tunneling in 3D waveguides of variable cross-section
We consider an infinite three-dimensional waveguide that far from the coordinate origin coincides with a cylinder. The waveguide has two narrows of diameter \(\varepsilon\). The narrows play the role of effective potential barriers for the longitudinal electron motion. The part of waveguide between...
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Published in | arXiv.org |
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Main Authors | , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
05.11.2013
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Subjects | |
Online Access | Get full text |
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Summary: | We consider an infinite three-dimensional waveguide that far from the coordinate origin coincides with a cylinder. The waveguide has two narrows of diameter \(\varepsilon\). The narrows play the role of effective potential barriers for the longitudinal electron motion. The part of waveguide between the narrows becomes a "resonator"\, and there can arise conditions for electron resonant tunneling. A magnetic field in the resonator can change the basic characteristics of this phenomenon. In the presence of a magnetic field, the tunneling phenomenon is feasible for producing spin-polarized electron flows consisting of electrons with spins of the same direction. We assume that the whole domain occupied by a magnetic field is in the resonator. An electron wave function satisfies the Pauli equation in the waveguide and vanishes at its boundary. Taking \(\varepsilon\) as a small parameter, we derive asymptotics for the probability \(T(E)\) of an electron with energy \(E\) to pass through the resonator, for the "resonant energy"\,\(E_{res}\), where \(T(E)\) takes its maximal value, and for some other resonant tunneling characteristics. |
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ISSN: | 2331-8422 |