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dc.contributor.authorCHUU, DSen_US
dc.contributor.authorHSIAO, CMen_US
dc.contributor.authorMEI, WNen_US
dc.date.accessioned2019-04-03T06:37:35Z-
dc.date.available2019-04-03T06:37:35Z-
dc.date.issued1992-08-15en_US
dc.identifier.issn0163-1829en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.46.3898en_US
dc.identifier.urihttp://hdl.handle.net/11536/3319-
dc.description.abstractThe energies of hydrogenic impurity states with an impurity atom located at the center of a quantum dot and on the axis of a quantum-well wire are studied. These two systems are all assumed to have an infinite confining potential. In the case of the quantum dot, the impurity eigenfunctions are expressed in terms of Whittaker functions and Coulomb scattering functions. The calculated ground-state energy of the impurity approaches the correct limit of three-dimensional hydrogen atom as the radius of the quantum dot becomes very large. In the case of the quantum-well wire, analytical solutions can be obtained if we divide the space into a two-dimensional subspace (perpendicular to the axis of the quantum-well wire) and a one-dimensional subspace (parallel to the axis of the quantum-well wire). The calculated ground-state energy of the quantum-well wire approaches the ground-state energy of the shallow-impurity atom located on the surface as the radius of the wire becomes infinite. Variations of the state energies with the radius of the quantum dot and the quantum-well wire are obtained.en_US
dc.language.isoen_USen_US
dc.titleHYDROGENIC IMPURITY STATES IN QUANTUM DOTS AND QUANTUM WIRESen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.46.3898en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume46en_US
dc.citation.issue7en_US
dc.citation.spage3898en_US
dc.citation.epage3905en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:A1992JJ84600025en_US
dc.citation.woscount224en_US
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