Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/81328
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dc.contributorPhotonics Research Centre-
dc.contributorDepartment of Electronic and Information Engineering-
dc.creatorWei, W-
dc.creatorYan, X-
dc.creatorShen, B-
dc.creatorZhang, X-
dc.date.accessioned2019-09-20T00:55:04Z-
dc.date.available2019-09-20T00:55:04Z-
dc.identifier.issn1931-7573-
dc.identifier.urihttp://hdl.handle.net/10397/81328-
dc.language.isoenen_US
dc.publisherSpringeren_US
dc.rights© The Author(s). 2019 Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.en_US
dc.rightsThe following publication Wei, W., Yan, X., Shen, B., & Zhang, X. (2019). Plasmon-induced transparency in an asymmetric bowtie structure. Nanoscale Research Letters, 14, 246, 1-6 is available at https://dx.doi.org/10.1186/s11671-019-3081-0en_US
dc.subjectSurface plasmonsen_US
dc.subjectPlasmon-induced transparencyen_US
dc.subjectElectromagnetically induced transparencyen_US
dc.subjectMetal-insulator-metalen_US
dc.titlePlasmon-induced transparency in an asymmetric bowtie structureen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1-
dc.identifier.epage6-
dc.identifier.volume14-
dc.identifier.doi10.1186/s11671-019-3081-0-
dcterms.abstractPlasmon-induced transparency is an efficient way to mimic electromagnetically induced transparency, which can eliminate the opaque effect of medium to the propagating electromagnetic wave. We proposed an aperture-side-coupled asymmetric bowtie structure to realize on-chip plasmon-induced transparency in optical communications band. The plasmon-induced transparency results from the strong coupling between the detuned bowtie triangular resonators. Either of the resonator works as a Fabry-Perot cavity with compact dimensions. The transparent peak wavelength can be easily controlled due to its strong linear relation with the resonator height. The ratio of absorption valley to the transparent peak can be more than 10dB. Moreover, with excellent linearity of shifting wavelength to sensing material index, the device has great sensing performance and immunity to the structure deviations.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationNanoscale research letters, 23 July 2019, v. 14, 246, p. 1-6-
dcterms.isPartOfNanoscale research letters-
dcterms.issued2019-
dc.identifier.isiWOS:000477036100003-
dc.identifier.scopus2-s2.0-85069530527-
dc.identifier.pmid31338743-
dc.identifier.eissn1556-276X-
dc.identifier.artn246-
dc.description.validate201909 bcrc-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Scopus/WOSen_US
dc.description.pubStatusPublisheden_US
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