Please use this identifier to cite or link to this item: http://cmuir.cmu.ac.th/jspui/handle/6653943832/68049
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dc.contributor.authorNontapat Wanwiengen_US
dc.contributor.authorChaiyawat Kaewmeechaien_US
dc.contributor.authorYongyut Laosiritawornen_US
dc.contributor.authorAtchara Punya Jaroenjittichaien_US
dc.date.accessioned2020-04-02T15:18:01Z-
dc.date.available2020-04-02T15:18:01Z-
dc.date.issued2019-12-16en_US
dc.identifier.issn17426596en_US
dc.identifier.issn17426588en_US
dc.identifier.other2-s2.0-85077820331en_US
dc.identifier.other10.1088/1742-6596/1380/1/012115en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85077820331&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/68049-
dc.description.abstract© Published under licence by IOP Publishing Ltd. We investigated electronic structures of CsPb(X x Y1-x)3 perovskites, where X, Y = Cl, Br, or I, and x = 0, 1/3, or 2/3, based on the density functional theory (DFT) with generalized gradient approximation (GGA). The results show that these materials exhibit direct and inverted gaps, in the sense that the character of electronic states near the valence band maximum (VBM) is derived from atomic s-like orbital of Pb and p-like orbital of halide atom, whereas the character of states near the conduction band minimum (CBM) is derived from atomic p-like orbital of Pb in contrast with the electronic band structures of other common semiconductors. Their density of states also indicates that the optical transition in both absorption and luminescence are stronger.en_US
dc.subjectPhysics and Astronomyen_US
dc.titleElectronic structures of CsPb(X <inf>x</inf> Y<inf>1-x</inf>)<inf>3</inf> perovskitesen_US
dc.typeConference Proceedingen_US
article.title.sourcetitleJournal of Physics: Conference Seriesen_US
article.volume1380en_US
article.stream.affiliationsChiang Mai Universityen_US
Appears in Collections:CMUL: Journal Articles

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