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dc.contributor.authorLi, Z.en_US
dc.contributor.authorGokkavas, M.en_US
dc.contributor.authorÖzbay, Ekmelen_US
dc.date.accessioned2016-02-08T09:37:48Z
dc.date.available2016-02-08T09:37:48Z
dc.date.issued2013en_US
dc.identifier.issn21951071
dc.identifier.urihttp://hdl.handle.net/11693/20909
dc.description.abstractAsymmetric transmissions of circularly polarized optical waves can be achieved when the waves are incident normal to planar chiral structures, provided that the structures are anisotropic and lossy. In order to clarify how the factor of loss affects the asymmetric transmission, Z. Li, M. Gokkavas, and E. Ozbay studied a typical planar chiral structure by using an optical lumped element model. On page 482, they found that the anisotropy of loss, instead of the whole loss, plays a crucial role for achieving asymmetric transmission. © 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.en_US
dc.language.isoEnglishen_US
dc.source.titleAdvanced Optical Materialsen_US
dc.relation.isversionofhttp://dx.doi.org/10.1002/adom.201370043en_US
dc.subjectAsymmetric transmissionen_US
dc.subjectChiral structuresen_US
dc.subjectMetamaterialsen_US
dc.subjectOptical nanostructuresen_US
dc.subjectPlasmonicsen_US
dc.titleChiral Structures: Manipulation of Asymmetric Transmission in Planar Chiral Nanostructures by Anisotropic Loss (Advanced Optical Materials 7/2013)en_US
dc.typeArticleen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.citation.spage472en_US
dc.citation.epage472en_US
dc.citation.volumeNumber1en_US
dc.citation.issueNumber7en_US
dc.identifier.doi10.1002/adom.201370043en_US
dc.contributor.bilkentauthorÖzbay, Ekmel
buir.contributor.orcidÖzbay, Ekmel|0000-0003-2953-1828en_US


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