Пожалуйста, используйте этот идентификатор, чтобы цитировать или ссылаться на этот ресурс: http://elar.urfu.ru/handle/10995/101667
Полная запись метаданных
Поле DCЗначениеЯзык
dc.contributor.authorSolovyev, I. V.en
dc.contributor.authorStreltsov, S. V.en
dc.date.accessioned2021-08-31T14:58:49Z-
dc.date.available2021-08-31T14:58:49Z-
dc.date.issued2019-
dc.identifier.citationSolovyev I. V. Microscopic toy model for magnetoelectric effect in polar Fe2Mo3O8 / I. V. Solovyev, S. V. Streltsov. — DOI 10.1103/PhysRevMaterials.3.114402 // Physical Review Materials. — 2019. — Vol. 3. — Iss. 11. — 114402.en
dc.identifier.issn24759953-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85075268122&doi=10.1103%2fPhysRevMaterials.3.114402&partnerID=40&md5=72e48c0ce6950851593ec4eacf78360b
dc.identifier.otherhttp://arxiv.org/pdf/1908.04946m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101667-
dc.description.abstractThe kamiokite Fe2Mo3O8 is regarded as a promising material exhibiting a giant magnetoelectric (ME) effect at the relatively high temperature T. Here, we explore this phenomenon on the basis of first-principles electronic structure calculations. For this purpose, we construct a realistic model describing the behavior of magnetic Fe 3d electrons and further map it onto the isotropic spin model. Our analysis suggests two possible scenarios for Fe2Mo3O8. The first one is based on the homogeneous charge distribution of the Fe2+ ions among tetrahedral (t) and octahedral (o) sites, which tends to lower the crystallographic P63mc symmetry through the formation of an orbitally ordered state. Nevertheless, the effect of the orbital ordering on interatomic exchange interactions does not seem to be strong, so that the magnetic properties can be described reasonably well by averaged interactions obeying the P63mc symmetry. The second scenario, which is supported by obtained parameters of on-site Coulomb repulsion and respects the P63mc symmetry, implies the charge disproportionation involving the somewhat exotic 1+ ionization state of the t-Fe sites (and 3+ state of the o-Fe sites). Somewhat surprisingly, these scenarios are practically indistinguishable from the viewpoint of exchange interactions, which are nearly identical in these two cases. However, the spin-dependent properties of the electric polarization are expected to be different due to the strong difference in the polarity of the Fe2+-Fe2+ and Fe1+-Fe3+ bonds. Our analysis uncovers the basic aspects of the ME effect in Fe2Mo3O8. Nevertheless, the quantitative description should involve other ingredients, apparently related to the lattice and orbitals degrees of freedom. © 2019 American Physical Society.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePhysic. Rev. Mat.2
dc.sourcePhysical Review Materialsen
dc.subjectCALCULATIONSen
dc.subjectDEGREES OF FREEDOM (MECHANICS)en
dc.subjectELECTRONIC STRUCTUREen
dc.subjectEXCHANGE INTERACTIONSen
dc.subjectCHARGE DISPROPORTIONATIONen
dc.subjectCOULOMB REPULSIONSen
dc.subjectELECTRIC POLARIZATIONen
dc.subjectFIRST PRINCIPLES ELECTRONIC STRUCTUREen
dc.subjectGIANT MAGNETOELECTRICen
dc.subjectINTERATOMIC EXCHANGE INTERACTIONSen
dc.subjectIONIZATION STATEen
dc.subjectQUANTITATIVE DESCRIPTIONen
dc.subjectIRON COMPOUNDSen
dc.titleMicroscopic toy model for magnetoelectric effect in polar Fe2Mo3O8en
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1103/PhysRevMaterials.3.114402-
dc.identifier.scopus85075268122-
local.contributor.employeeSolovyev, I.V., International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan, Department of Theoretical Physics and Applied Mathematics, Ural Federal University, Mira str. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeStreltsov, S.V., Department of Theoretical Physics and Applied Mathematics, Ural Federal University, Mira str. 19, Ekaterinburg, 620002, Russian Federation, Institute of Metal Physics, S. Kovalevskaya str. 18, Ekaterinburg, 620108, Russian Federation
local.issue11-
local.volume3-
local.contributor.departmentInternational Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan
local.contributor.departmentDepartment of Theoretical Physics and Applied Mathematics, Ural Federal University, Mira str. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentInstitute of Metal Physics, S. Kovalevskaya str. 18, Ekaterinburg, 620108, Russian Federation
local.identifier.pure11348998-
local.identifier.pure4a057a31-3a4d-48f1-95fc-a78d10d79be7uuid
local.description.order114402-
local.identifier.eid2-s2.0-85075268122-
Располагается в коллекциях:Научные публикации, проиндексированные в SCOPUS и WoS CC

Файлы этого ресурса:
Файл Описание РазмерФормат 
2-s2.0-85075268122.pdf1,84 MBAdobe PDFПросмотреть/Открыть


Все ресурсы в архиве электронных ресурсов защищены авторским правом, все права сохранены.