Asymmetric transmission of terahertz waves using polar dielectrics
buir.contributor.author | Özbay, Ekmel | |
buir.contributor.orcid | Özbay, Ekmel|0000-0003-2953-1828 | |
dc.citation.epage | 3088 | en_US |
dc.citation.issueNumber | 3 | en_US |
dc.citation.spage | 3075 | en_US |
dc.citation.volumeNumber | 22 | en_US |
dc.contributor.author | Serebryannikov, A. E. | en_US |
dc.contributor.author | Özbay, Ekmel | en_US |
dc.contributor.author | Nojima, S. | en_US |
dc.date.accessioned | 2015-07-28T11:57:37Z | |
dc.date.available | 2015-07-28T11:57:37Z | |
dc.date.issued | 2014-02-10 | en_US |
dc.department | Department of Physics | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.description.abstract | Asymmetric 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 America | en_US |
dc.description.provenance | Made 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.doi | 10.1364/OE.22.003075 | en_US |
dc.identifier.issn | 1094-4087 | |
dc.identifier.uri | http://hdl.handle.net/11693/11420 | |
dc.language.iso | English | en_US |
dc.publisher | Optical Society of America | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1364/OE.22.003075 | en_US |
dc.source.title | Optics Express | en_US |
dc.subject | Photonic Crystals | en_US |
dc.subject | Unidirectional Transmission | en_US |
dc.subject | Nonsymmetric Gratings | en_US |
dc.subject | Excitonic Polaritons | en_US |
dc.subject | Optical Isolator | en_US |
dc.subject | Propagation | en_US |
dc.subject | Refraction | en_US |
dc.subject | Index | en_US |
dc.subject | Diode | en_US |
dc.title | Asymmetric transmission of terahertz waves using polar dielectrics | en_US |
dc.type | Article | en_US |
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