Multiple slow waves and relevant transverse transmission and confinement in chirped photonic crystals

dc.contributor.author Serebryannikov, Andriy E.
dc.contributor.author Cakmak, A. Ozgur
dc.contributor.author Colak, Evrim
dc.contributor.author Caglayan, Humeyra
dc.contributor.author Kurt, Hamza
dc.contributor.author Ozbay, Ekmel
dc.contributor.department AGÜ, Mühendislik Fakültesi, Elektrik & Elektronik Mühendisliği Bölümü en_US
dc.contributor.institutionauthor
dc.date.accessioned 2020-02-14T11:42:06Z
dc.date.available 2020-02-14T11:42:06Z
dc.date.issued 2014 en_US
dc.description This work is supported by the projects DPT-HAMIT, ESF-EPIGRAT, and NATO-SET-181, and by TUBITAK under Project Nos., 107A004, 109A015, 109E301, and 110T306. A.E.S. thanks TUBITAK for partial support in the framework of the Visiting Researcher Program. H.K. and E.O. acknowledge partial support from the Turkish Academy of Sciences. en_US
dc.description.abstract The dispersion properties of rod-type chirped photonic crystals (PhCs) and non-channeled transmission in the direction of the variation of structural parameters from one cell of such a PhC to another are studied. Two types of configurations that enable multiple slow waves but differ in the utilized chirping scheme are compared. It is demonstrated that the multiple, nearly flat bands with a group index of refraction exceeding 180 can be obtained. For these bands, transmission is characterized by multiple narrow peaks of perfect transmission, strong field enhancement inside the slab, and large values of the Q-factor. Among the bands, there are some that show negative phase velocity. Symmetry with respect to the slab mid-plane must be kept in order to obtain constructive interferences that are necessary for reflection-free transmission. It is shown that 15 and more slow wave bands can be obtained in one configuration. The corresponding transmission peaks are well separated from each other, being the only significant feature of the transmission spectrum, while the Q-factor can exceed 10(5). The observed features are preserved in a wide range of the incidence angle variation. They can be used for tuning the locations and spectral widths of the transmission peaks. Some comparisons with the chirped multilayer structures have been carried out. (C) 2014 Optical Society of America en_US
dc.description.sponsorship Turkiye Cumhuriyeti Kalkinma Bakanligi ESF-EPIGRAT Turkiye Bilimsel ve Teknolojik Arastirma Kurumu (TUBITAK) 107A004 109A015 109E301 110T306 Turkish Academy of Sciences NATO-SET-181 en_US
dc.identifier.doi 10.1364/OE.22.021806
dc.identifier.issn 1094-4087
dc.identifier.other DOI: 10.1364/OE.22.021806
dc.identifier.uri https://hdl.handle.net/20.500.12573/165
dc.language.iso eng en_US
dc.publisher OPTICAL SOC AMER, 2010 MASSACHUSETTS AVE NW, WASHINGTON, DC 20036 USA en_US
dc.relation.ispartofseries Volume: 22 Issue: 18 Pages: 21806-21819;
dc.relation.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
dc.rights info:eu-repo/semantics/openAccess en_US
dc.subject LIGHT en_US
dc.subject GUIDES en_US
dc.subject LOCALIZATION en_US
dc.subject RESONATOR en_US
dc.title Multiple slow waves and relevant transverse transmission and confinement in chirped photonic crystals en_US
dc.type article en_US

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