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dc.contributor.authorKashin, I. V.en
dc.contributor.authorMazurenko, V. V.en
dc.contributor.authorKatsnelson, M. I.en
dc.contributor.authorRudenko, A. N.en
dc.date.accessioned2021-08-31T14:58:05Z-
dc.date.available2021-08-31T14:58:05Z-
dc.date.issued2020-
dc.identifier.citationOrbitally-resolved ferromagnetism of monolayer CrI3 / I. V. Kashin, V. V. Mazurenko, M. I. Katsnelson, et al. — DOI 10.1088/2053-1583/ab72d8 // 2D Materials. — 2020. — Vol. 7. — Iss. 2. — 025036.en
dc.identifier.issn20531583-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85082525308&doi=10.1088%2f2053-1583%2fab72d8&partnerID=40&md5=acb9040a912eae9384f94db8a3ddeb29
dc.identifier.otherhttp://arxiv.org/pdf/1912.11828m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101546-
dc.description.abstractFew-layer CrI3 is the most known example among two-dimensional (2D) ferromagnets, which have attracted growing interest in recent years. Despite considerable efforts and progress in understanding the properties of 2D magnets both from theory and experiment, the mechanism behind the formation of in-plane magnetic ordering in chromium halides is still under debate. Here, we propose a microscopic orbitally-resolved description of ferromagnetism in monolayer CrI3. Starting from first-principles calculations, we construct a low-energy model for the isotropic Heisenberg exchange interactions. We find that there are two competing contributions to the long-range magnetic ordering in CrI3: (i) Antiferromagnetic Anderson's superexchange between half-filled t 2g orbitals of Cr atoms; and (ii) Ferromagnetic exchange governed by the Kugel-Khomskii mechanism, involving the transitions between half-filled t 2g and empty e g orbitals. Using numerical calculations, we estimate the exchange interactions in momentum-space, which allows us to restore the spin-wave spectrum, as well as estimate the Curie temperature. Contrary to the nearest-neighbor effective models, our calculations suggest the presence of sharp resonances in the spin-wave spectrum at 5-7 meV, depending on the vertical bias voltage. Our estimation of the Curie temperature in monolayer CrI3 yields 55-65 K, which is in good agreement with experimental data. © 2020 IOP Publishing Ltd.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherIOP Publishing Ltden
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.source2D Materials2
dc.source2D Materialsen
dc.subjectCRI3en
dc.subjectDENSITY FUNCTIONAL THEORYen
dc.subjectELECTRIC FIELD EFFECTSen
dc.subjectEXCHANGE INTERACTIONSen
dc.subjectMAGNETIC-FORCE THEOREMen
dc.subjectTRICHALCOGENIDESen
dc.subjectTWO-DIMENSIONAL MATERIALSen
dc.subjectANTIFERROMAGNETISMen
dc.subjectCALCULATIONSen
dc.subjectCHROMIUM COMPOUNDSen
dc.subjectCURIE TEMPERATUREen
dc.subjectDENSITY FUNCTIONAL THEORYen
dc.subjectELECTRIC FIELD EFFECTSen
dc.subjectEXCHANGE INTERACTIONSen
dc.subjectFERROMAGNETIC MATERIALSen
dc.subjectFERROMAGNETISMen
dc.subjectMAGNETIC FIELD EFFECTSen
dc.subjectMAGNETSen
dc.subjectMONOLAYERSen
dc.subjectSPIN WAVESen
dc.subjectCRI3en
dc.subjectFERROMAGNETIC EXCHANGEen
dc.subjectFIRST-PRINCIPLES CALCULATIONen
dc.subjectLONG RANGE MAGNETIC ORDERen
dc.subjectMAGNETIC FORCEen
dc.subjectNUMERICAL CALCULATIONen
dc.subjectTRICHALCOGENIDESen
dc.subjectTWO-DIMENSIONAL MATERIALSen
dc.subjectIODINE COMPOUNDSen
dc.titleOrbitally-resolved ferromagnetism of monolayer CrI3en
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/2053-1583/ab72d8-
dc.identifier.scopus85082525308-
local.contributor.employeeKashin, I.V., Theoretical Physics and Applied Mathematics Department, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeMazurenko, V.V., Theoretical Physics and Applied Mathematics Department, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeKatsnelson, M.I., Theoretical Physics and Applied Mathematics Department, Ural Federal University, Ekaterinburg, 620002, Russian Federation, Institute for Molecules and Materials, Radboud University, Heijendaalseweg 135, Nijmegen, 6525 AJ, Netherlands
local.contributor.employeeRudenko, A.N., Theoretical Physics and Applied Mathematics Department, Ural Federal University, Ekaterinburg, 620002, Russian Federation, Institute for Molecules and Materials, Radboud University, Heijendaalseweg 135, Nijmegen, 6525 AJ, Netherlands, School of Physics and Technology, Wuhan University, Wuhan, 430072, China
local.issue2-
local.volume7-
dc.identifier.wos000518947800001-
local.contributor.departmentTheoretical Physics and Applied Mathematics Department, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentInstitute for Molecules and Materials, Radboud University, Heijendaalseweg 135, Nijmegen, 6525 AJ, Netherlands
local.contributor.departmentSchool of Physics and Technology, Wuhan University, Wuhan, 430072, China
local.identifier.pure95dd97a8-a89b-4221-9fb3-8d547c244625uuid
local.identifier.pure12440186-
local.description.order025036-
local.identifier.eid2-s2.0-85082525308-
local.identifier.wosWOS:000518947800001-
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