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dc.contributor.authorChu, CSen_US
dc.contributor.authorTang, CSen_US
dc.date.accessioned2014-12-08T15:02:54Z-
dc.date.available2014-12-08T15:02:54Z-
dc.date.issued1996-01-01en_US
dc.identifier.issn0038-1098en_US
dc.identifier.urihttp://dx.doi.org/10.1016/0038-1098(95)00597-8en_US
dc.identifier.urihttp://hdl.handle.net/11536/1505-
dc.description.abstractThe quantum transport in a narrow channel (NC) is studied in the presence of a time-dependent delta-profile electric field. The electric field is taken to be transversely polarized, with frequency omega, causing inter-subband and inter-sideband transitions Suppression in the de conductance G is found, which escalates with the chemical potential. There are structures in G which are related to the quasi-bound state (QBS) features. Major dip, and dip-and-peak, structures occur when an incident electron makes transition to a subband edge by absorbing or emitting one, and two, h omega, respectively. Structures associated with 3h omega processes are recognized. The QBS are closely associated with the singular density of states (DOS) at subband bottoms. Our results demonstrate that, due to this singular features of the DOS, the interaction of the electron with the electric field has to be treated beyond finite order perturbation.en_US
dc.language.isoen_USen_US
dc.subjectnanostructuresen_US
dc.subjectsemiconductorsen_US
dc.subjectelectronic transporten_US
dc.subjectradiation effectsen_US
dc.titleEffects of a time-dependent transverse electric field on the quantum transport in narrow channelsen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/0038-1098(95)00597-8en_US
dc.identifier.journalSOLID STATE COMMUNICATIONSen_US
dc.citation.volume97en_US
dc.citation.issue2en_US
dc.citation.spage119en_US
dc.citation.epage123en_US
dc.contributor.department交大名義發表zh_TW
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentNational Chiao Tung Universityen_US
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:A1996TF73200009-
dc.citation.woscount10-
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