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dc.contributor.authorUshakov, A. V.en
dc.contributor.authorStreltsov, S. V.en
dc.contributor.authorKhomskii, D. I.en
dc.date.accessioned2021-08-31T14:59:39Z-
dc.date.available2021-08-31T14:59:39Z-
dc.date.issued2019-
dc.identifier.citationUshakov A. V. Structural transition in AuAgTe4 under pressure / A. V. Ushakov, S. V. Streltsov, D. I. Khomskii. — DOI 10.1088/1361-648X/ab0b8a // Journal of Physics Condensed Matter. — 2019. — Vol. 31. — Iss. 23. — 235601.en
dc.identifier.issn9538984-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85064723151&doi=10.1088%2f1361-648X%2fab0b8a&partnerID=40&md5=efaca4cdfde4bb6e4cd3849739e4f756
dc.identifier.otherhttp://arxiv.org/pdf/1812.04862m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101774-
dc.description.abstractGold is inert and forms very few compounds. One of the most interesting of those is calaverite AuTe2, which has incommensurate structure and which becomes superconducting when doped or under pressure. There exist a 'sibling' of AuTe2, the mineral sylvanite AuAgTe4, which properties are almost unknown. In sylvanite Au and Ag ions are ordered in stripes, and Te6 octahedra around metals are distorted in such a way that Ag becomes linearly coordinated, what is typical for Ag1+ , whereas Au is square coordinated - it is typical for d 8 configurations, i.e. one can assign to Au the valence 3+. Our theoretical study shows that at pressure GPa there should occur in it a structural transition such that above this critical pressure Te6 octahedra around Au and Ag become regular and practically identical. Simultaneously Te-Te dimers, existing at P = 0 GPa, disappear, and material from a bad metal becomes a usual metal with predominantly Te 5p states at the Fermi energy. We expect that, similar to AuTe2, AuAgTe4 should become superconducting above . © 2019 IOP Publishing Ltd.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherInstitute of Physics Publishingen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceJ Phys Condens Matter2
dc.sourceJournal of Physics Condensed Matteren
dc.subjectELECTRONIC STRUCTUREen
dc.subjectHIGH-PRESSURE PHASEen
dc.subjectSTRUCTURAL TRANSITIONen
dc.subjectSYLVANITEen
dc.subjectELECTRONIC STRUCTUREen
dc.subjectGOLDen
dc.subjectGOLD COMPOUNDSen
dc.subjectSILVERen
dc.subjectBAD METALSen
dc.subjectCRITICAL PRESSURESen
dc.subjectHIGH-PRESSURE PHASEen
dc.subjectINCOMMENSURATE STRUCTUREen
dc.subjectSTRUCTURAL TRANSITIONSen
dc.subjectSYLVANITEen
dc.subjectTHEORETICAL STUDYen
dc.subjectTELLURIUM COMPOUNDSen
dc.titleStructural transition in AuAgTe4 under pressureen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/1361-648X/ab0b8a-
dc.identifier.scopus85064723151-
local.contributor.employeeUshakov, A.V., M.N. Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeStreltsov, S.V., M.N. Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, Ekaterinburg, 620108, Russian Federation, Ural Federal University, Mira St. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeKhomskii, D.I., II. Physikalisches Institut, Universitaet zu Koeln, Zuelpicher str. 77, Koeln, 50937, Germany
local.issue23-
local.volume31-
dc.identifier.wos000463108400001-
local.contributor.departmentM.N. Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, Ekaterinburg, 620108, Russian Federation
local.contributor.departmentUral Federal University, Mira St. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentII. Physikalisches Institut, Universitaet zu Koeln, Zuelpicher str. 77, Koeln, 50937, Germany
local.identifier.pure9314552-
local.description.order235601-
local.identifier.eid2-s2.0-85064723151-
local.identifier.wosWOS:000463108400001-
local.identifier.pmid30818287-
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