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Complete determination of the crystallographic orientation of ReX2 (X = S, Se) by polarized Raman spectroscopy

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dc.contributor.authorChoi, Y-
dc.contributor.authorKim, K-
dc.contributor.authorLim, SY-
dc.contributor.authorKim, J-
dc.contributor.authorPark, JM-
dc.contributor.authorJung Hwa Kim-
dc.contributor.authorZonghoon Lee-
dc.contributor.authorCheong, H-
dc.date.available2020-07-06T06:43:55Z-
dc.date.created2020-03-17-
dc.date.issued2020-02-
dc.identifier.issn2055-6756-
dc.identifier.urihttps://pr.ibs.re.kr/handle/8788114/7176-
dc.description.abstractPolarized Raman spectroscopy on few-layer ReS2 and ReSe2 was carried out to determine the crystallographic orientations. Since monolayer ReX2 (X = S or Se) has a distorted trigonal structure with only an inversion center, there is in-plane anisotropy and the two faces of a monolayer crystal are not equivalent. Since many physical properties vary sensitively depending on the crystallographic orientation, it is important to develop a reliable method to determine the crystal axes of ReX2. By comparing the relative polarization dependences of some representative Raman modes measured with three different excitation laser energies with high-resolution scanning transmission electron microscopy, we established a reliable procedure to determine all three principal directions of few-layer ReX2, including a way to distinguish the two types of faces: a 2.41 eV laser for ReS2 or a 1.96 eV laser for ReSe2 should be chosen as the excitation source of polarized Raman measurements; then the relative directions of the maximum intensity polarization of the Raman modes at 151 and 212 cm(-1) (124 and 161 cm(-1)) of ReS2 (ReSe2) can be used to determine the face types and the Re-chain direction unambiguously. ©The Royal Society of Chemistry 2020-
dc.description.uri1-
dc.language영어-
dc.publisherROYAL SOC CHEMISTRY-
dc.titleComplete determination of the crystallographic orientation of ReX2 (X = S, Se) by polarized Raman spectroscopy-
dc.typeArticle-
dc.type.rimsART-
dc.identifier.wosid000511441800007-
dc.identifier.scopusid2-s2.0-85079181070-
dc.identifier.rimsid71576-
dc.contributor.affiliatedAuthorJung Hwa Kim-
dc.contributor.affiliatedAuthorZonghoon Lee-
dc.identifier.doi10.1039/c9nh00487d-
dc.identifier.bibliographicCitationNANOSCALE HORIZONS, v.5, no.2, pp.308 - 315-
dc.citation.titleNANOSCALE HORIZONS-
dc.citation.volume5-
dc.citation.number2-
dc.citation.startPage308-
dc.citation.endPage315-
dc.description.journalClass1-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.subject.keywordPlusFEW-LAYER RES2-
dc.subject.keywordPlusATOMICALLY THIN-
dc.subject.keywordPlusCRYSTAL-STRUCTURE-
dc.subject.keywordPlusPHASE DIFFERENCE-
dc.subject.keywordPlusRHENIUM-
dc.subject.keywordPlusTRANSITION-
dc.subject.keywordPlusDEPENDENCE-
dc.subject.keywordPlusSCATTERING-
dc.subject.keywordPlusSEMICONDUCTOR-
dc.subject.keywordPlusANISOTROPY-
Appears in Collections:
Center for Multidimensional Carbon Materials(다차원 탄소재료 연구단) > 1. Journal Papers (저널논문)
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