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dc.contributor.authorHsue, YCen_US
dc.contributor.authorYang, TJen_US
dc.date.accessioned2014-12-08T15:39:40Z-
dc.date.available2014-12-08T15:39:40Z-
dc.date.issued2004-02-01en_US
dc.identifier.issn0038-1098en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.ssc.2003.11.023en_US
dc.identifier.urihttp://hdl.handle.net/11536/27091-
dc.description.abstractThe plane wave method is normally applied to determine the eigenfrequency of a two-dimensional (2D) photonic crystal. A slight change to this eigenvalue equation makes the wave number its eigenvalue providing a direct means to determine the attenuated length of the evanescent modes at the frequency within the photonic band gap. The contour of the length of attenuation of the evanescent modes in a square lattice can be determined using the proposed wave number eigenvalue equation. The wave number eigenvalue equation for the two-dimensional (3D) photonic crystal can also be obtained using a derivation similar to that for the 2D photonic crystal. Possible applications of the proposed calculation-method are presented. (C) 2003 Elsevier Ltd. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectphotonic crystalen_US
dc.subjectsquare latticeen_US
dc.subjectattenuated lengthen_US
dc.subjectwave number eigenvalueen_US
dc.titleContour of the attenuated length of an evanescent wave at constant frequency within a band gap of photonic crystalen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.ssc.2003.11.023en_US
dc.identifier.journalSOLID STATE COMMUNICATIONSen_US
dc.citation.volume129en_US
dc.citation.issue7en_US
dc.citation.spage475en_US
dc.citation.epage478en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000188735600012-
dc.citation.woscount10-
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