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dc.contributor.authorLi, Z.en_US
dc.contributor.authorGokkavas, M.en_US
dc.contributor.authorÖzbay, Ekmelen_US
dc.date.accessioned2016-02-08T09:37:51Z
dc.date.available2016-02-08T09:37:51Z
dc.date.issued2013en_US
dc.identifier.issn2195-1071
dc.identifier.urihttp://hdl.handle.net/11693/20912
dc.description.abstractPlanar chiral structures may provide asymmetric transmission for circularly polarized optical waves at normal incidence if the structures are anisotropic and lossy, but the role of loss has not yet been clarified. Here, a typical planar chiral structure is studied, and the mechanism of asymmetric transmission is analyzed. It is demonstrated for the first time that asymmetric transmission can be manipulated by changing the anisotropy of loss.en_US
dc.language.isoEnglishen_US
dc.source.titleAdvanced Optical Materialsen_US
dc.relation.isversionofhttp://dx.doi.org/10.1002/adom.201300183en_US
dc.subjectAsymmetric transmissionen_US
dc.subjectChiral structuresen_US
dc.subjectMetamaterialsen_US
dc.subjectOptical nanostructuresen_US
dc.subjectPlasmonicsen_US
dc.titleManipulation of Asymmetric Transmission in Planar Chiral Nanostructures by Anisotropic Lossen_US
dc.typeArticleen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentNanotechnology Research Center (NANOTAM)en_US
dc.citation.spage482en_US
dc.citation.epage488en_US
dc.citation.volumeNumber1en_US
dc.citation.issueNumber7en_US
dc.identifier.doi10.1002/adom.201300183en_US
dc.publisherWileyen_US
dc.contributor.bilkentauthorÖzbay, Ekmelen_US


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