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dc.contributor.authorAkgöl, Oğuzhan
dc.contributor.authorÜnal, Emin
dc.contributor.authorAltıntaş, Olcay
dc.contributor.authorKaraaslan, Muharrem
dc.contributor.authorKaradağ, Faruk
dc.contributor.authorSabah, Cumali
dc.date.accessioned12.07.201910:50:10
dc.date.accessioned2019-07-12T22:06:28Z
dc.date.available12.07.201910:50:10
dc.date.available2019-07-12T22:06:28Z
dc.date.issued2018
dc.identifier.citationAkgol, O., Unal, E., Altintas, O., Karaaslan, M., Karadag, F., Sabah, C. (2018). Design of metasurface polarization converter from linearly polarized signal to circularly polarized signal. Optik, 161, pp. 12-19. https://doi.org/10.1016/j.ijleo.2018.02.028en_US
dc.identifier.issn0030-4026
dc.identifier.urihttps://doi.org/10.1016/j.ijleo.2018.02.028
dc.identifier.urihttps://hdl.handle.net/20.500.12508/724
dc.descriptionWOS: 000429499100003en_US
dc.description.abstractIn this study, we both numerically and experimentally present a metasurface (MS) polarization converter to transform linearly polarized signal into circularly polarized one. The unit cell consists of two rectangular metallic patches placed at the crossed corners of rectangularly arranged inclusions. The results of a full-wave Electromagnetic (EM) simulator are compared to those of free space measurement using two horn antenna at microwave frequency regime. For a linearly polarized antenna, the s-parameters are obtained for both co-polarized and cross-polarized responses. The polarization quality referred to as axial ratio (AR) is expressed by the ratio of these two responses. It is found that, strong polarization conversion activity is obtained with the proposed MS at the frequency of about 3 GHz. As a result, we can generate polarization converter with a wide bandwidth, of interest for microwave filtering, coating, and especially polarization conversion devices. (C) 2018 Elsevier GmbH. All rights reserved.en_US
dc.description.sponsorshipScientific and Technological Research Council of Turkey (TUBITAK) [114E295, 113E290]en_US
dc.description.sponsorshipThis study is supported by the Scientific and Technological Research Council of Turkey (TUBITAK) under the grant numbers of 114E295 and 113E290.en_US
dc.language.isoengen_US
dc.publisherElsevier GmbHen_US
dc.relation.isversionof10.1016/j.ijleo.2018.02.028en_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectMetasurfaceen_US
dc.subjectPolarization conversionen_US
dc.subjectAxial ratioen_US
dc.subject.classificationOpticsen_US
dc.subject.classificationBerry Phase | Hologram | Terahertz Waveen_US
dc.subject.otherMetamaterialen_US
dc.subject.otherResonatorsen_US
dc.subject.otherSurfaceen_US
dc.subject.otherIndexen_US
dc.subject.otherCircular polarizationen_US
dc.subject.otherHorn antennasen_US
dc.subject.otherMathematical transformationsen_US
dc.subject.otherScattering parametersen_US
dc.subject.otherAxial ratioen_US
dc.subject.otherCircularly polarizeden_US
dc.subject.otherElectromagnetic simulatorsen_US
dc.subject.otherFree space measurementsen_US
dc.subject.otherLinearly polarized antennasen_US
dc.subject.otherPolarization convertersen_US
dc.subject.otherMicrowave filtersen_US
dc.titleDesign of metasurface polarization converter from linearly polarized signal to circularly polarized signalen_US
dc.typearticleen_US
dc.relation.journalOptiken_US
dc.contributor.departmentMühendislik ve Doğa Bilimleri Fakültesi -- Elektrik-Elektronik Mühendisliği Bölümüen_US
dc.contributor.authorID0000-0003-3237-4392en_US
dc.contributor.authorID0000-0001-7862-9085en_US
dc.contributor.authorID0000-0002-4346-3537en_US
dc.identifier.volume161en_US
dc.identifier.startpage12en_US
dc.identifier.endpage19en_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.contributor.isteauthorAkgöl, Oğuzhanen_US
dc.contributor.isteauthorÜnal, Eminen_US
dc.contributor.isteauthorAltıntaş, Olcayen_US
dc.contributor.isteauthorKaraaslan, Muharremen_US
dc.relation.indexWeb of Science - Scopusen_US
dc.relation.indexWeb of Science Core Collection - Science Citation Index Expandeden_US


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