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Characteristics of Thin Hf-Silicate Gate Dielectrics after Remote N-2 and N2O Plasma Post-Treatments

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dc.contributor.authorKim, Hyungchul-
dc.contributor.authorKim, Seokhoon-
dc.contributor.authorWoo, Sanghyun-
dc.contributor.authorChung, Hye Yeong-
dc.contributor.authorKim, Honggyu-
dc.contributor.authorPark, Jongsan-
dc.contributor.authorJeon, Hyeongtag-
dc.date.accessioned2022-12-21T00:59:03Z-
dc.date.available2022-12-21T00:59:03Z-
dc.date.created2022-08-26-
dc.date.issued2008-10-
dc.identifier.issn0013-4651-
dc.identifier.urihttps://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/177823-
dc.description.abstractWe investigated the thermal stability and physical properties of nitrided Hf-silicate after applying N-2 and N2O plasma treatments. The Hf-silicate film was created by remote-plasma atomic layer deposition using Hf[N(CH3)C2H5](4) and Si[N(CH3)](3)H as source gases and O-2 plasma as the oxidant. After rapid thermal annealing in N-2 ambient, the Hf silicate crystallized at 800 degrees C, while Hf-silicate films after the N-2 and N2O plasma treatments remained amorphous after annealing at 800 degrees C. Remote-plasma treatment of Hf-silicate resulted in a shift of the O 1s peaks to a lower binding energy. The increase in peak intensities of the Si-O-N, Si-O-Hf, and Si-O bonds at the interface after annealing was higher after N2O plasma treatment than after N-2 plasma treatment. The accumulation capacitances of an as-grown Hf-silicate metal-oxide-semiconductor structure after N-2 plasma treatment show that it has a better capacitance density (280 pF) than the same structure after N2O plasma treatment (235 pF). The equivalent oxide thickness values for the Hf-silicate films after N-2 and N2O plasma treatments are 3.36 and 3.8 nm, respectively.-
dc.language영어-
dc.language.isoen-
dc.publisherELECTROCHEMICAL SOC INC-
dc.titleCharacteristics of Thin Hf-Silicate Gate Dielectrics after Remote N-2 and N2O Plasma Post-Treatments-
dc.typeArticle-
dc.contributor.affiliatedAuthorJeon, Hyeongtag-
dc.identifier.doi10.1149/1.2990702-
dc.identifier.scopusid2-s2.0-54949085474-
dc.identifier.wosid000260479700066-
dc.identifier.bibliographicCitationJOURNAL OF THE ELECTROCHEMICAL SOCIETY, v.155, no.12, pp.G299 - G303-
dc.relation.isPartOfJOURNAL OF THE ELECTROCHEMICAL SOCIETY-
dc.citation.titleJOURNAL OF THE ELECTROCHEMICAL SOCIETY-
dc.citation.volume155-
dc.citation.number12-
dc.citation.startPageG299-
dc.citation.endPageG303-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaElectrochemistry-
dc.relation.journalResearchAreaMaterials Science-
dc.relation.journalWebOfScienceCategoryElectrochemistry-
dc.relation.journalWebOfScienceCategoryMaterials Science, Coatings & Films-
dc.subject.keywordPlusELECTRICAL-PROPERTIES-
dc.subject.keywordPlusTHERMAL-STABILITY-
dc.subject.keywordPlusFILMS-
dc.subject.keywordPlusLAYER-
dc.subject.keywordPlusNITROGEN-
dc.identifier.urlhttps://iopscience.iop.org/article/10.1149/1.2990702-
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