Electrically controllable plasmon induced reflectance in hybrid metamaterials

buir.contributor.authorÖzbay, Ekmel
buir.contributor.authorHabib, Mohsin
buir.contributor.authorGökbayrak, Murat
buir.contributor.orcidÖzbay, Ekmel|0000-0003-2953-1828
dc.citation.epage221105-4en_US
dc.citation.issueNumber22en_US
dc.citation.spage221105-1en_US
dc.citation.volumeNumber113en_US
dc.contributor.authorHabib, Mohsinen_US
dc.contributor.authorGökbayrak, Muraten_US
dc.contributor.authorÖzbay, Ekmelen_US
dc.contributor.authorCağlayan, H.en_US
dc.date.accessioned2019-02-21T16:02:58Z
dc.date.available2019-02-21T16:02:58Z
dc.date.issued2018en_US
dc.departmentNanotechnology Research Center (NANOTAM)en_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.description.abstractThe tunable plasmon induced reflectance (PIR) effect has been numerically investigated and experimentally realized by hybrid metal-graphene metamaterials. The PIR effect is produced by two parallel strips of gold (Au) and controlled electrically by applying the gate voltage to the graphene layer. The PIR response is generated by the weak hybridization of two bright modes of the gold strips and tuned by changing the Fermi level (Ef) of the graphene. The total shift of 211.7 nm was achieved in the reflection peak by applying only 3 V. This concept of real time electrical tuning of PIR, with a modulation depth of ∼49% and a spectral contrast ratio of 66.6%, can be used for designing optical switches, optical modulators, and tunable sensors.
dc.identifier.doi10.1063/1.5063461
dc.identifier.issn0003-6951
dc.identifier.urihttp://hdl.handle.net/11693/50061
dc.language.isoEnglish
dc.publisherAmerican Institute of Physics
dc.relation.isversionofhttps://doi.org/10.1063/1.5063461
dc.source.titleApplied Physics Lettersen_US
dc.titleElectrically controllable plasmon induced reflectance in hybrid metamaterialsen_US
dc.typeArticleen_US

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