Broadband circular polarizer based on high-contrast gratings
buir.contributor.author | Özbay, Ekmel | |
buir.contributor.orcid | Özbay, Ekmel|0000-0003-2953-1828 | |
dc.citation.epage | 2096 | en_US |
dc.citation.issueNumber | 11 | en_US |
dc.citation.spage | 2094 | en_US |
dc.citation.volumeNumber | 37 | en_US |
dc.contributor.author | Mutlu, M. | en_US |
dc.contributor.author | Akosman, A. E. | en_US |
dc.contributor.author | Özbay, Ekmel | en_US |
dc.date.accessioned | 2016-02-08T09:46:28Z | |
dc.date.available | 2016-02-08T09:46:28Z | |
dc.date.issued | 2012-05-30 | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Nanotechnology Research Center (NANOTAM) | en_US |
dc.description.abstract | A circular polarizer, which is composed of periodic and two-dimensional dielectric high-contrast gratings, is designed theoretically such that a unity conversion efficiency is achieved at λ0 = 1.55 μm. The operation is obtained by the achievement of the simultaneous unity transmission of transverse magnetic and transverse electric waves with a phase difference of π/2, meaning that an optimized geometrical anisotropy is accomplished. By the utilization of the rigorous coupled-wave analysis and finite-difference time-domain methods, it is shown that a percent bandwidth of ∼50% can be achieved when the operation bandwidth is defined as the wavelengths for which the conversion efficiency exceeds 0.9. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T09:46:28Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2012 | en |
dc.identifier.doi | 10.1364/OL.37.002094 | en_US |
dc.identifier.issn | 0146-9592 | |
dc.identifier.uri | http://hdl.handle.net/11693/21445 | |
dc.language.iso | English | en_US |
dc.publisher | Optical Society of America | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1364/OL.37.002094 | en_US |
dc.source.title | Optics Letters | en_US |
dc.subject | Circular polarizers | en_US |
dc.subject | Finite-difference time-domain (FDTD) methods | en_US |
dc.subject | Geometrical anisotropy | en_US |
dc.subject | High contrast | en_US |
dc.subject | Operation bandwidth | en_US |
dc.subject | Phase difference | en_US |
dc.subject | Rigorous coupled wave analysis | en_US |
dc.subject | Transverse electric waves | en_US |
dc.subject | Transverse magnetic | en_US |
dc.subject | Circular polarization | en_US |
dc.subject | Conversion efficiency | en_US |
dc.subject | Electromagnetic waves | en_US |
dc.subject | Finite difference time domain method | en_US |
dc.subject | Diffraction gratings | en_US |
dc.title | Broadband circular polarizer based on high-contrast gratings | en_US |
dc.type | Article | en_US |
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