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dc.contributor.authorPan, CLen_US
dc.contributor.authorHsieh, CFen_US
dc.contributor.authorPan, RPen_US
dc.contributor.authorTanaka, Men_US
dc.contributor.authorMiyamaru, Fen_US
dc.contributor.authorTani, Men_US
dc.contributor.authorHangyo, Men_US
dc.date.accessioned2014-12-08T15:19:05Z-
dc.date.available2014-12-08T15:19:05Z-
dc.date.issued2005-05-30en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OPEX.13.003921en_US
dc.identifier.urihttp://hdl.handle.net/11536/13695-
dc.description.abstractWe demonstrate frequency tuning of enhanced THz radiation transmitted through a two- dimensional metallic hole array ( 2D- MHA) by controlling the index of refraction of the medium filling the holes and adjacent to the 2D- MHA on one side. The medium is a nematic liquid crystal ( NLC) and its index of refraction is varied using magnetically controlled birefringence of the NLC. With the NLC, the peak transmission frequency of the 2D- MHA shift to the red by 0.112 THz and can be tuned from 0.193 to 0.188 THz. The peak transmittance is as high as 70% or an enhancement of 2.42 times, considering the porosity of the 2D- MHA. As a tunable THz filter, this device exhibits a continuous tuning range of 4.7 GHz, a low insertion loss of 2.35 to 1.55 dB and a quality factor of similar to 4- 5. (C) 2005 Optical Society of America.en_US
dc.language.isoen_USen_US
dc.titleControl of enhanced THz transmission through metallic hole arrays using nematic liquid crystalen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OPEX.13.003921en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume13en_US
dc.citation.issue11en_US
dc.citation.spage3921en_US
dc.citation.epage3930en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000229534500003-
dc.citation.woscount66-
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