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dc.contributor.authorAbdeldaim, A. H.en
dc.contributor.authorLi, T.en
dc.contributor.authorFarrar, L.en
dc.contributor.authorTsirlin, A. A.en
dc.contributor.authorYao, W.en
dc.contributor.authorGibbs, A. S.en
dc.contributor.authorManuel, P.en
dc.contributor.authorLightfoot, P.en
dc.contributor.authorNilsen, Gø. J.en
dc.contributor.authorClark, L.en
dc.date.accessioned2022-05-12T08:12:55Z-
dc.date.available2022-05-12T08:12:55Z-
dc.date.issued2020-
dc.identifier.citationRealizing Square and Diamond Lattice S=1/2 Heisenberg Antiferromagnet Models in the α and β Phases of the Coordination Framework, KTi(C2 O4)2·x H2O / A. H. Abdeldaim, T. Li, L. Farrar et al. // Physical Review Materials. — 2020. — Vol. 4. — Iss. 10. — 104414.en
dc.identifier.issn2475-9953-
dc.identifier.otherAll Open Access, Green3
dc.identifier.urihttp://elar.urfu.ru/handle/10995/111101-
dc.description.abstractWe report the crystal structures and magnetic properties of two pseudopolymorphs of the S=1/2 Ti3+ coordination framework, KTi(C2O4)2·xH2O. Single-crystal x-ray and powder neutron diffraction measurements on α-KTi(C2O4)2·xH2O confirm its structure in the tetragonal I4/mcm space group with a square planar arrangement of Ti3+ ions. Magnetometry and specific heat measurements reveal weak antiferromagnetic interactions, with J1≈7 K and J2/J1=0.11 indicating a slight frustration of nearest- and next-nearest-neighbor interactions. Below 1.8 K, α-KTi(C2O4)2·xH2O undergoes a transition to G-type antiferromagnetic order with magnetic moments aligned along the c axis of the tetragonal structure. The estimated ordered moment of Ti3+ in α-KTi(C2O4)2·xH2O is suppressed from its spin-only value to 0.62(3)μB, thus verifying the two-dimensional nature of the magnetic interactions within the system. β-KTi(C2O4)2·2H2O, on the other hand, realizes a three-dimensional diamondlike magnetic network of Ti3+ moments within a hexagonal P6222 structure. An antiferromagnetic exchange coupling of J≈54 K - an order of magnitude larger than in α-KTi(C2O4)2·xH2O - is extracted from magnetometry and specific heat data. β-KTi(C2O4)2·2H2O undergoes Néel ordering at TN=28 K, with the magnetic moments aligned within the ab plane and a slightly reduced ordered moment of 0.79μB per Ti3+. Through density-functional theory calculations, we address the origin of the large difference in the exchange parameters between the α and β pseudopolymorphs. Given their observed magnetic behaviors, we propose α-KTi(C2O4)2·xH2O and β-KTi(C2O4)2·2H2O as close to ideal model S=1/2 Heisenberg square and diamond lattice antiferromagnets, respectively. © 2020 American Physical Society.en
dc.description.sponsorshipProvision of a Ph.D. studentship to A.H.A. by the University of Liverpool and the Science and Technology Facilities Council (STFC) is gratefully acknowledged. The work of T.L. was funded by the University of St Andrews and China Scholarship Council (CSC) joint scholarship (201606280032). A.T. was funded by the Federal Ministry of Education and Research through the Sofja Kovalevskaya Award of Alexander von Humboldt Foundation. Work at St Andrews was supported by the Leverhulme Trust (RPG-2013-343). The authors are also grateful to the STFC for access to neutron beamtime at ISIS and thank Dr. Gavin Stenning for aiding with SQUID and specific heat measurements at the Materials Characterization Laboratory, ISIS. We thank Dr. Manh Duc Le (ISIS), Dr. Ross Stewart (ISIS), Dr. Craig Robertson (Uni. Liverpool), Dr. Samantha Chong (Uni. Liverpool), and Dr. Hamish Yeung (Uni. Birmingham) for useful discussions.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Physical Societyen1
dc.publisherAmerican Physical Society (APS)en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePhysic. Rev. Mat.2
dc.sourcePhysical Review Materialsen
dc.subjectANTIFERROMAGNETIC MATERIALSen
dc.subjectANTIFERROMAGNETISMen
dc.subjectCRYSTAL LATTICESen
dc.subjectDENSITY FUNCTIONAL THEORYen
dc.subjectDIAMONDSen
dc.subjectMAGNETIC MOMENTSen
dc.subjectMAGNETOMETERSen
dc.subjectMAGNETOMETRYen
dc.subjectSINGLE CRYSTALSen
dc.subjectSPECIFIC HEATen
dc.subjectSPIN FLUCTUATIONSen
dc.subjectTHERMAL VARIABLES MEASUREMENTen
dc.subjectANTIFERRO-MAGNETIC INTERACTIONSen
dc.subjectANTIFERROMAGNETIC EXCHANGE COUPLINGen
dc.subjectANTIFERROMAGNETIC ORDERINGSen
dc.subjectCOORDINATION FRAMEWORKSen
dc.subjectHEISENBERG ANTIFERROMAGNETSen
dc.subjectNEXT NEAREST NEIGHBOR INTERACTIONen
dc.subjectPOWDER NEUTRON DIFFRACTIONen
dc.subjectTWO DIMENSIONAL NATUREen
dc.subjectTITANIUM COMPOUNDSen
dc.titleRealizing Square and Diamond Lattice S=1/2 Heisenberg Antiferromagnet Models in the α and β Phases of the Coordination Framework, KTi(C2 O4)2·x H2Oen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/acceptedVersionen
dc.identifier.doi10.1103/PhysRevMaterials.4.104414-
dc.identifier.scopus85095433240-
local.contributor.employeeAbdeldaim, A.H., Department of Chemistry and Materials Innovation Factory, University of Liverpool, 51 Oxford Street, Liverpool, L7 3NY, United Kingdom, School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom, Isis Neutron and Muon Source, Science and Technology Facilities Council, Didcot, OX11 0QX, United Kingdom; Li, T., School of Chemistry, University of St. Andrews, St. Andrews, KY16 9ST, United Kingdom; Farrar, L., Department of Chemistry and Materials Innovation Factory, University of Liverpool, 51 Oxford Street, Liverpool, L7 3NY, United Kingdom; Tsirlin, A.A., Theoretical Physics and Applied Mathematics Department, Ural Federal University, Yekaterinburg, 620002, Russian Federation, Experimental Physics Vi, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, Augsburg, 86135, Germany; Yao, W., School of Chemistry, University of St. Andrews, St. Andrews, KY16 9ST, United Kingdom, Functional Thin Films Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, 518055, China; Gibbs, A.S., Isis Neutron and Muon Source, Science and Technology Facilities Council, Didcot, OX11 0QX, United Kingdom; Manuel, P., Isis Neutron and Muon Source, Science and Technology Facilities Council, Didcot, OX11 0QX, United Kingdom; Lightfoot, P., School of Chemistry, University of St. Andrews, St. Andrews, KY16 9ST, United Kingdom; Nilsen, Gø.J., Isis Neutron and Muon Source, Science and Technology Facilities Council, Didcot, OX11 0QX, United Kingdom; Clark, L., Department of Chemistry and Materials Innovation Factory, University of Liverpool, 51 Oxford Street, Liverpool, L7 3NY, United Kingdom, School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdomen
local.issue10-
local.volume4-
dc.identifier.wos000619240300001-
local.contributor.departmentDepartment of Chemistry and Materials Innovation Factory, University of Liverpool, 51 Oxford Street, Liverpool, L7 3NY, United Kingdom; School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom; Isis Neutron and Muon Source, Science and Technology Facilities Council, Didcot, OX11 0QX, United Kingdom; School of Chemistry, University of St. Andrews, St. Andrews, KY16 9ST, United Kingdom; Theoretical Physics and Applied Mathematics Department, Ural Federal University, Yekaterinburg, 620002, Russian Federation; Experimental Physics Vi, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, Augsburg, 86135, Germany; Functional Thin Films Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, 518055, Chinaen
local.identifier.pure20131597-
local.description.order104414-
local.identifier.eid2-s2.0-85095433240-
local.identifier.wosWOS:000619240300001-
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