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dc.contributor.authorNikolaev, S. A.en
dc.contributor.authorSolovyev, I. V.en
dc.date.accessioned2021-08-31T14:57:09Z-
dc.date.available2021-08-31T14:57:09Z-
dc.date.issued2020-
dc.identifier.citationNikolaev S. A. Skyrmionic order and magnetically induced polarization change in lacunar spinel compounds GaV4 S8 and GaMo4 S8: Comparative theoretical study / S. A. Nikolaev, I. V. Solovyev. — DOI 10.1103/PhysRevB.102.014414 // Physical Review B. — 2020. — Vol. 102. — Iss. 1. — 014414.en
dc.identifier.issn24699950-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85091490492&doi=10.1103%2fPhysRevB.102.014414&partnerID=40&md5=e9d89588fcfaf39c38b86ae5f2f3f7cd
dc.identifier.otherhttp://arxiv.org/pdf/2004.11548m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101424-
dc.description.abstractWe show how low-energy electronic models derived from the first-principles electronic structure calculations can help to rationalize the magnetic properties of two lacunar spinel compounds GaM4S8 with relatively light (M=V) and heavy (M=Mo) transition-metal elements, which are responsible for different spin-orbit interaction strength. In the model, each magnetic lattice point was associated with the (M4S4)5+ molecule, and the model itself was formulated in the basis of molecular Wannier functions constructed for three magnetic t2 bands. The effects of rhombohedral distortion, spin-orbit interaction, band filling, and the screening of Coulomb interactions in the t2 bands are discussed in details by stressing similarities and differences between GaV4S8 and GaMo4S8. The electronic model is further treated in the superexchange approximation, which allows us to derive an effective spin model for the energy and electric polarization (P) depending on the relative orientation of spins in the bonds, and study the properties of this model by means of classical Monte Carlo simulations with the emphasis on the possible formation of the skyrmionic phase. While isotropic exchange interactions clearly dominate in GaV4S8, all types of interactions (isotropic, antisymmetric, and symmetric anisotropic) are comparable in the case of GaMo4S8. Particularly, large uniaxial exchange anisotropy has a profound effect on the properties of GaMo4S8. On the one hand, it raises the Curie temperature by opening a gap in the spectrum of magnon excitations. On the other hand, it strongly affects the skyrmionic phase by playing the role of a molecular field, which facilitates the formation of skyrmions, but makes them relatively insensitive to the external magnetic field in the large part of the phase diagram. We predict reversal of the magnetic dependence of P in the case of GaMo4S8 caused by the reversal of the direction of rhombohedral distortion. © 2020 American Physical Society.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePhys. Rev. B2
dc.sourcePhysical Review Ben
dc.subjectANISOTROPYen
dc.subjectBINARY ALLOYSen
dc.subjectCALCULATIONSen
dc.subjectELECTRONIC STRUCTUREen
dc.subjectELECTRONSen
dc.subjectMAGNETISMen
dc.subjectMONTE CARLO METHODSen
dc.subjectPOLARIZATIONen
dc.subjectTRANSITION METALSen
dc.subjectELECTRIC POLARIZATIONen
dc.subjectEXTERNAL MAGNETIC FIELDen
dc.subjectFIRST PRINCIPLES ELECTRONIC STRUCTUREen
dc.subjectINDUCED POLARIZATIONen
dc.subjectRELATIVE ORIENTATIONen
dc.subjectRHOMBOHEDRAL DISTORTIONen
dc.subjectSPIN ORBIT INTERACTIONSen
dc.subjectTRANSITION METAL ELEMENTSen
dc.subjectSPIN ORBIT COUPLINGen
dc.titleSkyrmionic order and magnetically induced polarization change in lacunar spinel compounds GaV4 S8 and GaMo4 S8: Comparative theoretical studyen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1103/PhysRevB.102.014414-
dc.identifier.scopus85091490492-
local.contributor.employeeNikolaev, S.A., Institute of Innovative Research, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama, 226-8503, Japan, National Institute for Materials Science, MANA, 1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan
local.contributor.employeeSolovyev, I.V., National Institute for Materials Science, MANA, 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, Institute of Metal Physics, S. Kovalevskaya str. 18, Ekaterinburg, 620108, Russian Federation
local.issue1-
local.volume102-
dc.identifier.wos000547333800003-
local.contributor.departmentInstitute of Innovative Research, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama, 226-8503, Japan
local.contributor.departmentNational Institute for Materials Science, MANA, 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.pure13400555-
local.description.order014414-
local.identifier.eid2-s2.0-85091490492-
local.identifier.wosWOS:000547333800003-
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