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Chemical state and atomic structure of Ge(2)Sb(2)Te(5) system for nonvolatile phase-change random access memory

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dc.contributor.authorJung, Min-Cherl-
dc.contributor.authorKim, Ki-Hong-
dc.contributor.authorLee, Young-Mi-
dc.contributor.authorEom, Jae-Hyeon-
dc.contributor.authorIm, Jino-
dc.contributor.authorYoon, Young-Gui-
dc.contributor.authorIhm, Jisoon-
dc.contributor.authorSong, Se Ahn-
dc.contributor.authorJeong, Hong-Sik-
dc.contributor.authorShin, Hyun-Joon-
dc.date.available2019-05-30T04:37:47Z-
dc.date.issued2008-10-
dc.identifier.issn0021-8979-
dc.identifier.issn1089-7550-
dc.identifier.urihttps://scholarworks.bwise.kr/cau/handle/2019.sw.cau/23594-
dc.description.abstractWe present chemical state information on contamination-free Ge(2)Sb(2)Te(5) thin film using high-resolution x-ray photoelectron spectroscopy (HRXPS) and the corresponding theoretical understanding of the chemical states, on both amorphous and metastable phases, illuminating the phase-change mechanism of the system. HRXPS data revealed that the Sb 4d shallow core level was split into two components having different binding energies and that the spin-orbit splitting feature of the Ge 3d level was enhanced as the system became metastable. Negligible change was observed in the Te 4d shallow core level, and in contrary to the previous report's prediction less change in valance band spectra was observed. The results imply that Sb movement is also involved in the phase-change mechanism and that acquisition of shallow core-level spectra can be a useful measure for understanding phase-change mechanism. Hydrogenated SbTe(6) octahedral-like cluster model was introduced to schematically interpret the generation of the two components in the Sb 4d level in metastable state, having an isotropic six-bonds configuration, and an anistropic six-bonds (three-short and three-elongated bonds) configuration. The amorphous state was modeled to have three-short bonds configuration. Finally, Stibnite-like building block model was used to show that the existence of the above two configurations for Sb atoms is feasible in the Ge(2)Sb(2)Te(5) system. (C) 2008 American Institute of Physics. [DOI: 10.1063/1.2990766]-
dc.language영어-
dc.language.isoENG-
dc.publisherAMER INST PHYSICS-
dc.titleChemical state and atomic structure of Ge(2)Sb(2)Te(5) system for nonvolatile phase-change random access memory-
dc.typeArticle-
dc.identifier.doi10.1063/1.2990766-
dc.identifier.bibliographicCitationJOURNAL OF APPLIED PHYSICS, v.104, no.7-
dc.description.isOpenAccessN-
dc.identifier.wosid000260125500163-
dc.identifier.scopusid2-s2.0-54049107309-
dc.citation.number7-
dc.citation.titleJOURNAL OF APPLIED PHYSICS-
dc.citation.volume104-
dc.type.docTypeArticle-
dc.publisher.location미국-
dc.subject.keywordPlusOPTICAL MEDIA-
dc.subject.keywordPlusFUTURE-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryPhysics, Applied-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
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