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dc.contributor.authorKim, Jun Ho-
dc.contributor.authorIm, Hyeong-Seop-
dc.contributor.authorHwang, Dae-Woong-
dc.contributor.authorKim, Sun-Kyung-
dc.contributor.authorBae, Dukkyu-
dc.contributor.authorYoo, Young-Zo-
dc.contributor.authorLee, Kyeong-Seok-
dc.contributor.authorSeong, Tae-Yeon-
dc.date.accessioned2024-01-20T02:02:41Z-
dc.date.available2024-01-20T02:02:41Z-
dc.date.created2021-09-01-
dc.date.issued2017-03-
dc.identifier.issn0272-8842-
dc.identifier.urihttps://pubs.kist.re.kr/handle/201004/123012-
dc.description.abstractHole-patterned Ag layers were first used to form Si-doped ZnO (SZO)/hole-patterned Ag/SZO multilayers and their optical and electrical properties were characterized. Unlike conventional oxide/metal/oxide multilayers, all samples exhibited two characteristic features: (i) a sinusoidal wavelength dependence of the transmittance with double maxima, and (ii) undulation in the visible transmittance, but not in the infrared transmittance. With increasing SZO thickness, the transmittance maxima were red-shifted, and the visible transmittance window widened. The carrier concentration decreased from 7.42x10(22) to 2.4x10(22) cm(-3), and the sheet resistances varied from 7 to 10 Omega/sq with increasing SZO thickness. Haacke's figure of merit (FOM) was calculated for the SZO-based multilayer films. The 40 nm-thick SZO multilayers had the highest FOM of 15.9x10(-3) Omega(-1). Finite difference time-domain (FDTD) simulations were undertaken to interpret the measured transmittance. Based on the FDTD simulations, the undulating transmittance was attributed to surface plasmon-polaritons.-
dc.languageEnglish-
dc.publisherELSEVIER SCI LTD-
dc.subjectROOM-TEMPERATURE-
dc.subjectLOW-RESISTANCE-
dc.subjectTHIN-FILMS-
dc.subjectELECTRODES-
dc.subjectOPTIMIZATION-
dc.subjectMETAL-
dc.subjectFIGURE-
dc.subjectPET-
dc.titleElectrical and optical characteristics of transparent conducting Si-doped. ZnO/hole-patterned Ag/Si-doped ZnO multilayer films-
dc.typeArticle-
dc.identifier.doi10.1016/j.ceramint.2016.11.213-
dc.description.journalClass1-
dc.identifier.bibliographicCitationCERAMICS INTERNATIONAL, v.43, no.4, pp.3693 - 3697-
dc.citation.titleCERAMICS INTERNATIONAL-
dc.citation.volume43-
dc.citation.number4-
dc.citation.startPage3693-
dc.citation.endPage3697-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.identifier.wosid000393937900031-
dc.identifier.scopusid2-s2.0-85007143198-
dc.relation.journalWebOfScienceCategoryMaterials Science, Ceramics-
dc.relation.journalResearchAreaMaterials Science-
dc.type.docTypeArticle-
dc.subject.keywordPlusROOM-TEMPERATURE-
dc.subject.keywordPlusLOW-RESISTANCE-
dc.subject.keywordPlusTHIN-FILMS-
dc.subject.keywordPlusELECTRODES-
dc.subject.keywordPlusOPTIMIZATION-
dc.subject.keywordPlusMETAL-
dc.subject.keywordPlusFIGURE-
dc.subject.keywordPlusPET-
dc.subject.keywordAuthorSi-doped ZnO-
dc.subject.keywordAuthorHole-patterned Ag layer-
dc.subject.keywordAuthorTransparent conducting electrode-
dc.subject.keywordAuthorFinite-difference time-domain simulation-
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