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dc.contributor.authorWan, X.en
dc.contributor.authorIvanov, V.en
dc.contributor.authorResta, G.en
dc.contributor.authorLeonov, I.en
dc.contributor.authorSavrasov, S. Y.en
dc.date.accessioned2021-08-31T15:07:25Z-
dc.date.available2021-08-31T15:07:25Z-
dc.date.issued2021-
dc.identifier.citationExchange interactions and sensitivity of the Ni two-hole spin state to Hund's coupling in doped NdNiO2 / X. Wan, V. Ivanov, G. Resta, et al. — DOI 10.1103/PhysRevB.103.075123 // Physical Review B. — 2021. — Vol. 103. — Iss. 7. — 075123.en
dc.identifier.issn24699950-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85100668913&doi=10.1103%2fPhysRevB.103.075123&partnerID=40&md5=0aaeabb0f3e4dbeb29ac5f41517708f8
dc.identifier.otherhttp://arxiv.org/pdf/2008.07465m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/103095-
dc.description.abstractUsing the density-functional-based LDA+U method and linear-response theory, we study the magnetic exchange interactions of the superconductor Nd1-xSrxNiO2. Our calculated nearest-neighbor exchange constant J1=82 meV is large, weakly affected by doping, and is only slightly smaller than that found in the sister compound CaCuO2. However, we find that the hole doping significantly enhances the interlayer exchange coupling as it affects the magnetic moment of the Ni-3d3z2-r2 orbital. This can be understood in terms of the small hybridization of Ni-3d3z2-r2 within the NiO2 plane, which results in a flat band near the Fermi level, and its large overlap along the z direction. We also demonstrate that the Nd-5d states appearing at the Fermi level do not affect the magnetic exchange interactions, and thus they may not participate in the superconductivity of this compound. Whereas many previous works emphasized the importance of the Ni-3dx2-y2 and Nd-5d orbitals, we analyze instead the solution of the Ni-3dx2-y2/Ni-3d3z2-r2 minimal model using dynamical mean field theory. It reveals an underlying Mott insulating state that, depending on the precise values of the intra-atomic Hund's coupling smaller or larger than 0.83 eV, selects upon doping either S=0 or 1 two-hole states at low energies, leading to very different quasiparticle band structures. We propose that trends upon doping in the spin excitation spectrum and the quasiparticle density of states can be a way to probe the Ni 3d8 configuration. © 2021 American Physical Society.en
dc.description.sponsorshipX.W. is supported by the NSFC (Grants No. 11834006, No. 11525417, No. 51721001, and No. 11790311), National Key R&D Program of China (Grants No. 2018YFA0305704 and No. 2017YFA0303203), and by 111 Project. X.W. also acknowledges the support from the Tencent Foundation through the XPLORER PRIZE. V.I., G.R., and S.Y.S. are supported by NSF DMR Grant No. 1832728. I.L. acknowledges support by the Russian Foundation for Basic Research (Project No. 18-32-20076). The DMFT electronic structure calculations were supported by the state assignment of Minobrnauki of Russia (theme “Electron” No. AAAA-A18-118020190098-5).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.subjectEXCHANGE INTERACTIONSen
dc.subjectFERMI LEVELen
dc.subjectMAGNETIC MOMENTSen
dc.subjectMEAN FIELD THEORYen
dc.subjectNICKELen
dc.subjectNICKEL OXIDEen
dc.subjectDENSITY FUNCTIONALSen
dc.subjectDYNAMICAL MEAN-FIELD THEORYen
dc.subjectINTERLAYER EXCHANGE COUPLINGen
dc.subjectLINEAR-RESPONSE THEORYen
dc.subjectMAGNETIC EXCHANGE INTERACTIONSen
dc.subjectMOTT-INSULATING STATEen
dc.subjectQUASIPARTICLE BAND STRUCTURESen
dc.subjectQUASIPARTICLE DENSITYen
dc.subjectEXCITED STATESen
dc.titleExchange interactions and sensitivity of the Ni two-hole spin state to Hund's coupling in doped NdNiO2en
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.rsi46750878-
dc.identifier.doi10.1103/PhysRevB.103.075123-
dc.identifier.scopus85100668913-
local.contributor.employeeWan, X., National Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
local.contributor.employeeIvanov, V., Department of Physics and Astronomy, University of California, Davis, CA 95616, United States
local.contributor.employeeResta, G., Department of Physics and Astronomy, University of California, Davis, CA 95616, United States
local.contributor.employeeLeonov, I., M. N. Miheev Institute of Metal Physics, Russian Academy of Sciences, Yekaterinburg, 620002, Russian Federation, Ural Federal University, Yekaterinburg, 620002, Russian Federation
local.contributor.employeeSavrasov, S.Y., Department of Physics and Astronomy, University of California, Davis, CA 95616, United States
local.issue7-
local.volume103-
dc.identifier.wos000617039500002-
local.contributor.departmentNational Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
local.contributor.departmentDepartment of Physics and Astronomy, University of California, Davis, CA 95616, United States
local.contributor.departmentM. N. Miheev Institute of Metal Physics, Russian Academy of Sciences, Yekaterinburg, 620002, Russian Federation
local.contributor.departmentUral Federal University, Yekaterinburg, 620002, Russian Federation
local.identifier.pure20889042-
local.identifier.puree1d5b1d7-79cc-46e4-9506-d2b1e58b83b6uuid
local.description.order075123-
local.identifier.eid2-s2.0-85100668913-
local.fund.rffi18-32-20076-
local.identifier.wosWOS:000617039500002-
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