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dc.contributor.authorUsseinov, A.en
dc.contributor.authorKoishybayeva, Z.en
dc.contributor.authorPlatonenko, A.en
dc.contributor.authorPankratov, V.en
dc.contributor.authorSuchikova, Y.en
dc.contributor.authorAkilbekov, A.en
dc.contributor.authorZdorovets, M.en
dc.contributor.authorPurans, J.en
dc.contributor.authorPopov, A. I.en
dc.date.accessioned2022-05-12T08:29:03Z-
dc.date.available2022-05-12T08:29:03Z-
dc.date.issued2021-
dc.identifier.citationVacancy Defects in Ga2O3: First-Principles Calculations of Electronic Structure / A. Usseinov, Z. Koishybayeva, A. Platonenko et al. // Materials. — 2021. — Vol. 14. — Iss. 23. — 7384.en
dc.identifier.issn1996-1944-
dc.identifier.otherAll Open Access, Green3
dc.identifier.urihttp://elar.urfu.ru/handle/10995/112123-
dc.description.abstractFirst-principles density functional theory (DFT) is employed to study the electronic structure of oxygen and gallium vacancies in monoclinic bulk β-Ga2 O3 crystals. Hybrid exchange– correlation functional B3LYP within the density functional theory and supercell approach were successfully used to simulate isolated point defects in β-Ga2 O3. Based on the results of our calcu-lations, we predict that an oxygen vacancy in β-Ga2 O3 is a deep donor defect which cannot be an effective source of electrons and, thus, is not responsible for n-type conductivity in β-Ga2 O3. On the other hand, all types of charge states of gallium vacancies are sufficiently deep acceptors with transition levels more than 1.5 eV above the valence band of the crystal. Due to high formation energy of above 10 eV, they cannot be considered as a source of p-type conductivity in β-Ga2 O3. © 2021 by the authors. Licensee MDPI, Basel, Switzerland.en
dc.description.sponsorshipFunding: This research was funded by the Science Committee of the Ministry of Education and Science of the Republic of Kazakhstan (Grant No. AP08856540) as well as by the Latvian research council via the Latvian National Research Program under the topic “High-Energy Physics and Accelerator Technologies”, Agreement No: VPP-IZM-CERN-2020/1-0002 for A.I. Popov. In addition, J. Purans is grateful to the ERAF project 1.1.1.1/20/A/057 while A. Platonenko was supported by Latvian Research Council No. LZP-2018/1-0214.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherMDPIen1
dc.publisherMDPI AGen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceMater.2
dc.sourceMaterialsen
dc.subjectDEEP DONORen
dc.subjectDFTen
dc.subjectOXYGEN VACANCYen
dc.subjectP-TYPE CONDUCTIVITYen
dc.subjectPOINT DEFECTSen
dc.subjectΒ-GA2 O3en
dc.subjectCALCULATIONSen
dc.subjectELECTRONIC STRUCTUREen
dc.subjectGALLIUMen
dc.subjectGALLIUM COMPOUNDSen
dc.subjectOXYGENen
dc.subjectOXYGEN VACANCIESen
dc.subjectPOINT DEFECTSen
dc.subjectDEEP DONORen
dc.subjectDENSITY-FUNCTIONAL-THEORYen
dc.subjectELECTRONIC.STRUCTUREen
dc.subjectFIRST PRINCIPLE CALCULATIONSen
dc.subjectFIRST-PRINCIPLE DENSITY-FUNCTIONAL THEORIESen
dc.subjectHYBRID EXCHANGEen
dc.subjectMONOCLINICSen
dc.subjectP TYPE CONDUCTIVITYen
dc.subjectVACANCY DEFECTSen
dc.subjectΒ-GA2 O3en
dc.subjectDENSITY FUNCTIONAL THEORYen
dc.titleVacancy Defects in Ga2O3: First-Principles Calculations of Electronic Structureen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.3390/ma14237384-
dc.identifier.scopus85120752925-
local.contributor.employeeUsseinov, A., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Koishybayeva, Z., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Platonenko, A., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan, Institute of Solid State Physics, University of Latvia, 8 Kengaraga Str, Riga, LV-1063, Latvia; Pankratov, V., Institute of Solid State Physics, University of Latvia, 8 Kengaraga Str, Riga, LV-1063, Latvia; Suchikova, Y., Department of Physics and Methods of Teaching Physics, Berdyansk State Pedagogical University, Berdyansk, 71100, Ukraine; Akilbekov, A., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Zdorovets, M., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan, Department of Intelligent Information Technologies, Ural Federal University, Yekaterinburg, 620075, Russian Federation; Purans, J., Institute of Solid State Physics, University of Latvia, 8 Kengaraga Str, Riga, LV-1063, Latvia; Popov, A.I., Faculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan, Institute of Solid State Physics, University of Latvia, 8 Kengaraga Str, Riga, LV-1063, Latviaen
local.issue23-
local.volume14-
dc.identifier.wos000743695200001-
local.contributor.departmentFaculty of Physics and Technical Sciences, L.N. Gumilyov, Eurasian National University, Nur-Sultan, 010008, Kazakhstan; Institute of Solid State Physics, University of Latvia, 8 Kengaraga Str, Riga, LV-1063, Latvia; Department of Physics and Methods of Teaching Physics, Berdyansk State Pedagogical University, Berdyansk, 71100, Ukraine; Department of Intelligent Information Technologies, Ural Federal University, Yekaterinburg, 620075, Russian Federationen
local.identifier.pure29147990-
local.description.order7384-
local.identifier.eid2-s2.0-85120752925-
local.fund.cordisH2020: 739508-
local.identifier.wosWOS:000743695200001-
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