Asymmetric transmission of terahertz waves using polar dielectrics

buir.contributor.authorÖzbay, Ekmel
buir.contributor.orcidÖzbay, Ekmel|0000-0003-2953-1828
dc.citation.epage3088en_US
dc.citation.issueNumber3en_US
dc.citation.spage3075en_US
dc.citation.volumeNumber22en_US
dc.contributor.authorSerebryannikov, A. E.en_US
dc.contributor.authorÖzbay, Ekmelen_US
dc.contributor.authorNojima, S.en_US
dc.date.accessioned2015-07-28T11:57:37Z
dc.date.available2015-07-28T11:57:37Z
dc.date.issued2014-02-10en_US
dc.departmentDepartment of Physicsen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.description.abstractAsymmetric wave transmission is a Lorentz reciprocal phenomenon, which can appear in the structures with broken symmetry. It may enable high forward-to-backward transmittance contrast, while transmission for one of the two opposite incidence directions is blocked. In this paper, it is demonstrated that ultrawideband, high-contrast asymmetric wave transmission can be obtained at terahertz frequencies in the topologically simple, i.e., one- or two-layer nonsymmetric gratings, which are entirely or partially made of a polar dielectric working in the ultralow-epsilon regime inspired by phonon-photon coupling. A variety of polar dielectrics with different characteristics can be used that gives one a big freedom concerning design. Simple criteria for estimating possible usefulness of a certain polar dielectric are suggested. Contrasts exceeding 80dB can be easily achieved without a special parameter adjustment. Stacking a high-e corrugated layer with a noncorrugated layer made of a polar dielectric, one can enhance transmission in the unidirectional regime. At large and intermediate angles of incidence, a better performance can be obtained owing to the common effect of nonsymmetric diffractions and directional selectivity, which is connected with the dispersion of the ultralow-e material. At normal incidence, strong asymmetry in transmission may occur in the studied structures as a purely diffraction effect. (C) 2014 Optical Society of Americaen_US
dc.description.provenanceMade available in DSpace on 2015-07-28T11:57:37Z (GMT). No. of bitstreams: 1 10.1364-OE.22.003075.pdf: 1374434 bytes, checksum: f5e3328b8ceafa2c6524a35380e34392 (MD5)en
dc.identifier.doi10.1364/OE.22.003075en_US
dc.identifier.issn1094-4087
dc.identifier.urihttp://hdl.handle.net/11693/11420
dc.language.isoEnglishen_US
dc.publisherOptical Society of Americaen_US
dc.relation.isversionofhttp://dx.doi.org/10.1364/OE.22.003075en_US
dc.source.titleOptics Expressen_US
dc.subjectPhotonic Crystalsen_US
dc.subjectUnidirectional Transmissionen_US
dc.subjectNonsymmetric Gratingsen_US
dc.subjectExcitonic Polaritonsen_US
dc.subjectOptical Isolatoren_US
dc.subjectPropagationen_US
dc.subjectRefractionen_US
dc.subjectIndexen_US
dc.subjectDiodeen_US
dc.titleAsymmetric transmission of terahertz waves using polar dielectricsen_US
dc.typeArticleen_US

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