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Effect of a ga-doped ZnO thin film with a ZTO buffer layer fabricated by using pulsed DC magnetron sputter for dye-sensitized solar cells

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dc.contributor.authorSong, Sang-Woo-
dc.contributor.authorLee, Kyung-Ju-
dc.contributor.authorRoh, Ji-Hyung-
dc.contributor.authorPark, On-Jeon-
dc.contributor.authorKim, Hwan-Sun-
dc.contributor.authorMoon, Byung-Moo-
dc.contributor.authorJi, Min-Woo-
dc.date.accessioned2021-09-05T06:38:22Z-
dc.date.available2021-09-05T06:38:22Z-
dc.date.created2021-06-15-
dc.date.issued2014-08-
dc.identifier.issn0374-4884-
dc.identifier.urihttps://scholar.korea.ac.kr/handle/2021.sw.korea/97896-
dc.description.abstractThe electrical property of a Ga-doped ZnO(GZO) thin film is well known to be similar that of commercialized fluorine-doped tin oxide(FTO). However GZO is limited for use at high process temperatures for solar cells because of its unstable resistivity at temperatures above 300 A degrees C. A GZO thin film compared to zinc tin oxide(ZTO)-GZO multilayer can be used at high process temperatures. A GZO thin film was deposited on glass by using pulsed DC magnetron sputter. Then, a ZTO buffer layer was deposited on the GZO surface. During the deposition, the working pressure was 5 mTorr (Z-1 glass) and 1 mTorr (Z-2 glass). Dye-sensitized solar cells (DSSCs) were fabricated using Z-1, Z-2 and commercialized FTO glasses. Z-2 showed a conversion efficiency of 4.265%, which was enhanced by 0.399% compared to that of the DSSCs using FTO(3.784%). The conversion efficiency for Z-1 (3.889%) was a little higher than that of FTO. Thus, the ZTO-GZO electrode showed better characteristics than those obtained using the FTO electrode, which can be attributed to the reduced charge recombination and series resistance.-
dc.languageEnglish-
dc.language.isoen-
dc.publisherKOREAN PHYSICAL SOC-
dc.subjectTRANSPARENT-
dc.subjectEFFICIENCY-
dc.titleEffect of a ga-doped ZnO thin film with a ZTO buffer layer fabricated by using pulsed DC magnetron sputter for dye-sensitized solar cells-
dc.typeArticle-
dc.contributor.affiliatedAuthorMoon, Byung-Moo-
dc.identifier.doi10.3938/jkps.65.308-
dc.identifier.scopusid2-s2.0-84907354210-
dc.identifier.wosid000340490000007-
dc.identifier.bibliographicCitationJOURNAL OF THE KOREAN PHYSICAL SOCIETY, v.65, no.3, pp.308 - 311-
dc.relation.isPartOfJOURNAL OF THE KOREAN PHYSICAL SOCIETY-
dc.citation.titleJOURNAL OF THE KOREAN PHYSICAL SOCIETY-
dc.citation.volume65-
dc.citation.number3-
dc.citation.startPage308-
dc.citation.endPage311-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.identifier.kciidART001900279-
dc.description.journalClass1-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.description.journalRegisteredClasskci-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryPhysics, Multidisciplinary-
dc.subject.keywordPlusTRANSPARENT-
dc.subject.keywordPlusEFFICIENCY-
dc.subject.keywordAuthorGZO-
dc.subject.keywordAuthorDye-sensitized solar cell-
dc.subject.keywordAuthorTCO-
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