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dc.contributor.authorMoser, H. O.en_US
dc.contributor.authorJian, L. K.en_US
dc.contributor.authorChen, H. S.en_US
dc.contributor.authorKalaiselvi, S. M. P.en_US
dc.contributor.authorVirasawmy, S.en_US
dc.contributor.authorCheng, X. X.en_US
dc.contributor.authorBanas, A.en_US
dc.contributor.authorBanas, K.en_US
dc.contributor.authorHeussler, S. P.en_US
dc.contributor.authorBahou, M.en_US
dc.contributor.authorWu, B. -I.en_US
dc.contributor.authorHua, Weien_US
dc.contributor.authorYi, Zhuen_US
dc.date.accessioned2019-04-03T06:47:37Z-
dc.date.available2019-04-03T06:47:37Z-
dc.date.issued2010-01-01en_US
dc.identifier.isbn978-0-8194-8184-9en_US
dc.identifier.issn0277-786Xen_US
dc.identifier.urihttp://dx.doi.org/10.1117/12.855094en_US
dc.identifier.urihttp://hdl.handle.net/11536/146277-
dc.description.abstractMeta-foils are all-metal free-standing electromagnetic metamaterials based on interconnected S-string architecture. They provide a versatile applications' platform. Lacking any substrate or embedding matrix, they feature arrays of parallel upright S-strings with each string longitudinally shifted by half an S compared to its neighbour to form capacitance-inductance loops. Geometric parameters include length a, width b, thickness t, and height h of an S, the gap between adjacent S-strings d, and the periodicity p of the interconnecting lines. Equidistant strings at p=1 form a 1SE meta-foil. Grouped in pairs of gap d, exhibiting a gap d(p) between pairs, they are named 2SP. Geometric parameters a, b, t, h, d, d(p), pS(E or P) and materials' properties like electric conductivity, Young's modulus, thermal expansion coefficient, and heat capacity determine the electromagnetic, mechanical, and thermal properties of meta-foils including the spectral dependence of resonance frequencies, refractive index, transmission, reflection, and bending. We show how the frequency and transmission of left-handed pass-bands depend on a, p, and d(p), the pSP geometry exhibiting higher resonance frequency and transmission. Equivalent circuit considerations serve to explain physical reasons. We also demonstrate mechanical behavior versus p and d(p) justifying the design of a cylindrical hyperlens depending on bent meta-foils.en_US
dc.language.isoen_USen_US
dc.subjectMeta-foilen_US
dc.subjectmetamaterialsen_US
dc.subjectfree-standingen_US
dc.subjectflexibleen_US
dc.subjectmicromanufacturingen_US
dc.subjectinfrared spectromicroscopyen_US
dc.subjecthyperlensen_US
dc.titleGeometry-function relationships in meta-foilsen_US
dc.typeProceedings Paperen_US
dc.identifier.doi10.1117/12.855094en_US
dc.identifier.journalMETAMATERIALS Ven_US
dc.citation.volume7711en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000285048300013en_US
dc.citation.woscount3en_US
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