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dc.contributor.authorHsieh, S. H.en_US
dc.contributor.authorChu, C. S.en_US
dc.date.accessioned2017-04-21T06:56:00Z-
dc.date.available2017-04-21T06:56:00Z-
dc.date.issued2016-01-18en_US
dc.identifier.issn0003-6951en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.4940684en_US
dc.identifier.urihttp://hdl.handle.net/11536/133549-
dc.description.abstractElectron injection into a graphene sheet through a slanted armchair graphene nanoribbon (AGNR) is investigated. An incident mode, or subband, in the AGNR is valley-unpolarized. Our attention is on the valley-resolved nature of the injected electron beams and its connection to the incident mode. It is known for a normal injection that an incident mode will split symmetrically into two valley-resolved beams of equal intensity. We show, in contrast, that slanted injections result in asymmetric valley-resolved beam splitting. The most asymmetric beam splitting cases, when one of the valley-resolved beams has basically disappeared, are found and the condition derived. This is shown not due to trigonal warping because it holds even in the low incident energy regime, as long as collimation allows. These most asymmetric beam splitting cases occur at energies within an energy interval near and include the subband edge of an incident mode. The physical picture is best illustrated by a projection of the slanted AGNR subband states onto that of the 2D graphene sheet. It follows that the disappearing of a valley-resolved beam coincides with the situation that the group velocities of the projected states in the corresponding valley are in backward directions. (C) 2016 AIP Publishing LLC.en_US
dc.language.isoen_USen_US
dc.titleAsymmetric valley-resolved beam splitting and incident modes in slanted graphene junctionsen_US
dc.identifier.doi10.1063/1.4940684en_US
dc.identifier.journalAPPLIED PHYSICS LETTERSen_US
dc.citation.volume108en_US
dc.citation.issue3en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000373055500050en_US
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