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Ekmekci, E.; Strikwerda, A. C.; Fan, K.; Keiser, G.; Zhang, X.; Turhan-Sayan, G.; Averitt, R. D.
<?xml version='1.0' encoding='utf-8'?> <oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"> <dc:creator>Ekmekci, E.</dc:creator> <dc:creator>Strikwerda, A. C.</dc:creator> <dc:creator>Fan, K.</dc:creator> <dc:creator>Keiser, G.</dc:creator> <dc:creator>Zhang, X.</dc:creator> <dc:creator>Turhan-Sayan, G.</dc:creator> <dc:creator>Averitt, R. D.</dc:creator> <dc:date>2011-01-01</dc:date> <dc:description>We present frequency tunable metamaterial designs at terahertz (THz) frequencies using broadside coupled split-ring resonator (BC-SRR) arrays. Frequency tuning, arising from changes in near-field coupling, is obtained by in-plane displacement of the two SRR layers. For electrical excitation, the resonance frequency continuously redshifts as a function of displacement. The maximum frequency shift occurs for vertical displacement of half a unit cell, resulting in a shift of 663 GHz (51% of f(0)). We discuss the difference in the BC-SRR response for electrical excitation in comparison to magnetic excitation in terms of hybridization arising from inductive and capacitive coupling.</dc:description> <dc:identifier>https://aperta.ulakbim.gov.trrecord/18415</dc:identifier> <dc:identifier>oai:zenodo.org:18415</dc:identifier> <dc:rights>info:eu-repo/semantics/openAccess</dc:rights> <dc:rights>http://www.opendefinition.org/licenses/cc-by</dc:rights> <dc:source>PHYSICAL REVIEW B 83(19)</dc:source> <dc:title>Frequency tunable terahertz metamaterials using broadside coupled split-ring resonators</dc:title> <dc:type>info:eu-repo/semantics/article</dc:type> <dc:type>publication-article</dc:type> </oai_dc:dc>
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