Single molecule magnet with an unpaired electron trapped between two lanthanide ions inside a fullerene

dc.bibliographicCitation.firstPage16098eng
dc.bibliographicCitation.journalTitleNature Communicationseng
dc.bibliographicCitation.lastPage2266eng
dc.bibliographicCitation.volume8eng
dc.contributor.authorLiu, F.
dc.contributor.authorKrylov, D.S.
dc.contributor.authorSpree, L.
dc.contributor.authorAvdoshenko, S.M.
dc.contributor.authorSamoylova, N.A.
dc.contributor.authorRosenkranz, M.
dc.contributor.authorKostanyan, A.
dc.contributor.authorGreber, T.
dc.contributor.authorWolter, A.U.B.
dc.contributor.authorBüchner, B.
dc.contributor.authorPopov, A.A.
dc.date.accessioned2020-07-20T06:05:22Z
dc.date.available2020-07-20T06:05:22Z
dc.date.issued2017
dc.description.abstractIncreasing the temperature at which molecules behave as single-molecule magnets is a serious challenge in molecular magnetism. One of the ways to address this problem is to create the molecules with strongly coupled lanthanide ions. In this work, endohedral metallofullerenes Y 2 @C 80 and Dy 2 @C 80 are obtained in the form of air-stable benzyl monoadducts. Both feature an unpaired electron trapped between metal ions, thus forming a single-electron metal-metal bond. Giant exchange interactions between lanthanide ions and the unpaired electron result in single-molecule magnetism of Dy 2 @C 80 (CH 2 Ph) with a record-high 100 s blocking temperature of 18 K. All magnetic moments in Dy 2 @C 80 (CH 2 Ph) are parallel and couple ferromagnetically to form a single spin unit of 21 μ B with a dysprosium-electron exchange constant of 32 cm -1. The barrier of the magnetization reversal of 613 K is assigned to the state in which the spin of one Dy centre is flipped.eng
dc.description.fondsLeibniz_Fonds
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://doi.org/10.34657/3691
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/5062
dc.language.isoengeng
dc.publisherLondon : Nature Publishing Groupeng
dc.relation.doihttps://doi.org/10.1038/ncomms16098
dc.relation.issn2041-1723
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subject.ddc530eng
dc.subject.otherfullereneeng
dc.subject.otherlanthanideeng
dc.subject.otherelectroneng
dc.subject.otherfullereneeng
dc.subject.otherfundamental particleeng
dc.subject.otherioneng
dc.subject.othermagnetizationeng
dc.subject.othermetaleng
dc.subject.othermolecular analysiseng
dc.subject.otherrare earth elementeng
dc.subject.otherArticleeng
dc.subject.otherchemical bondeng
dc.subject.otherchemical interactioneng
dc.subject.otherchemical reactioneng
dc.subject.othercrystal structureeng
dc.subject.otherdensity functional theoryeng
dc.subject.otherelectrochemical analysiseng
dc.subject.otherelectroneng
dc.subject.otherelectron spin resonanceeng
dc.subject.otherferromagnetic couplingeng
dc.subject.otherhysteresiseng
dc.subject.otherlow temperatureeng
dc.subject.othermagnetic fieldeng
dc.subject.othermagnetismeng
dc.subject.othermagnetometryeng
dc.subject.othermatrix-assisted laser desorption-ionization mass spectrometryeng
dc.subject.othermoleculeeng
dc.subject.otherparticle sizeeng
dc.subject.otherroom temperatureeng
dc.subject.othersynthesiseng
dc.subject.otherX ray diffractioneng
dc.titleSingle molecule magnet with an unpaired electron trapped between two lanthanide ions inside a fullereneeng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIFWDeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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