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Control of polarity and defects in the growth of AlN films on Si (111) surfaces by inserting an Al interlayer

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dc.contributor.authorLee, Sang-Tae-
dc.contributor.authorPark, Byung-Guon-
dc.contributor.authorKim, Moon-Deock-
dc.contributor.authorOh, Jae-Eung-
dc.contributor.authorKim, Song-Gang-
dc.contributor.authorKim, Young-Heon-
dc.contributor.authorYang, Woo-Chul-
dc.date.accessioned2021-06-23T07:53:30Z-
dc.date.available2021-06-23T07:53:30Z-
dc.date.issued2012-03-
dc.identifier.issn1567-1739-
dc.identifier.issn1878-1675-
dc.identifier.urihttps://scholarworks.bwise.kr/erica/handle/2021.sw.erica/33180-
dc.description.abstractWe discuss the role of the Al interlayer in the suppression of pinhole formations and also look at the polarity transition of the AlN layers from N-polarity to Al-polarity when this Al interlayer is present. The AlN layers were grown by molecular beam epitaxy on an AlN nucleation layer. A thin Al interlayer was deposited on the initial nucleated AlN layer after the nitridation of the Al-soaked Si (111) substrates. The AlN layer with an Al interlayer showed a relatively smooth surface with a reduced density of pinholes compared with the AlN layer grown without an Al interlayer. In addition, the AlN layer with an Al interlayer showed some stacking faults in the interface between the Si substrate and the A1N layer. We also identify the polarity change of the AlN layer after the insertion of a thin Al interlayer from N-polarity to Al-polarity by chemical etching. A simple model is constructed to explain the polarity change and the pinhole suppression due to the Al interlayer. (C) 2011 Elsevier B.V. All rights reserved.-
dc.format.extent4-
dc.language영어-
dc.language.isoENG-
dc.publisherELSEVIER SCIENCE BV-
dc.titleControl of polarity and defects in the growth of AlN films on Si (111) surfaces by inserting an Al interlayer-
dc.typeArticle-
dc.publisher.location네델란드-
dc.identifier.doi10.1016/j.cap.2011.07.034-
dc.identifier.scopusid2-s2.0-81155131084-
dc.identifier.wosid000297003600006-
dc.identifier.bibliographicCitationCURRENT APPLIED PHYSICS, v.12, no.2, pp 385 - 388-
dc.citation.titleCURRENT APPLIED PHYSICS-
dc.citation.volume12-
dc.citation.number2-
dc.citation.startPage385-
dc.citation.endPage388-
dc.type.docTypeArticle-
dc.identifier.kciidART001644321-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClasssci-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.description.journalRegisteredClasskci-
dc.relation.journalResearchAreaMaterials Science-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryMaterials Science, Multidisciplinary-
dc.relation.journalWebOfScienceCategoryPhysics, Applied-
dc.subject.keywordPlusGAN-
dc.subject.keywordPlusEPITAXY-
dc.subject.keywordPlusOVERGROWTH-
dc.subject.keywordPlusALXGA1-XN-
dc.subject.keywordPlusLAYER-
dc.subject.keywordAuthorAlN-
dc.subject.keywordAuthorAl interlayer-
dc.subject.keywordAuthorPolarity control-
dc.subject.keywordAuthorPinhole suppression-
dc.subject.keywordAuthorMolecular beam epitaxy-
dc.identifier.urlhttps://www.sciencedirect.com/science/article/pii/S1567173911004196?via%3Dihub-
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