Measurement of electron correlations in LixCoO2 (x=0.0–0.35) using 59Co nuclear magnetic resonance and nuclear quadrupole resonance techniques

dc.contributorAalto-yliopistofi
dc.contributorAalto Universityen
dc.contributor.authorKawasaki, S.
dc.contributor.authorMotohashi, T.
dc.contributor.authorShimada, K.
dc.contributor.authorOno, T.
dc.contributor.authorKanno, R.
dc.contributor.authorKarppinen, Maarit
dc.contributor.authorYamauchi, H.
dc.contributor.authorZheng, Guo-qing
dc.contributor.departmentKemian laitosfi
dc.contributor.departmentDepartment of Chemistryen
dc.contributor.schoolKemian tekniikan korkeakoulufi
dc.contributor.schoolSchool of Chemical Technologyen
dc.date.accessioned2015-10-06T09:02:11Z
dc.date.available2015-10-06T09:02:11Z
dc.date.issued2009
dc.description.abstractCoO2 is the parent compound for the superconductor NaxCoO2⋅1.3H2O and was widely believed to be a Mott insulator. We performed C59o nuclear magnetic resonance and nuclear quadrupole resonance studies on LixCoO2 (x=0.35, 0.25, 0.12, and 0.0) to uncover the electronic state and spin correlations in this series of compounds which was recently obtained through electrochemical deintercalation of Li from pristine LiCoO2. We find that although the antiferromagnetic spin correlations systematically increase with decreasing Li content (x), the end member, CoO2, is a noncorrelated metal that well satisfies the Korringa relation for a Fermi liquid. Thus, CoO2 is not simply located at the limit of x→0 for AxCoO2 (A=Li,Na) compounds. The disappearance of the electron correlations in CoO2 is due to the three dimensionality of the compound which is in contrast to the highly two-dimensional structure of AxCoO2.en
dc.description.versionPeer revieweden
dc.format.extent220514/1-4
dc.format.mimetypeapplication/pdfen
dc.identifier.citationKawasaki, S. & Motohashi, T. & Shimada, K. & Ono, T. & Kanno, R. & Karppinen, Maarit & Yamauchi, H. & Zheng, Guo-qing. 2009. Measurement of electron correlations in LixCoO2 (x=0.0-0.35) using 59Co nuclear magnetic resonance and nuclear quadrupole resonance techniques. Physical Review B. Volume 79, Issue 22. 220514/1-4. ISSN 1550-235X (electronic). DOI: 10.1103/physrevb.79.220514.en
dc.identifier.doi10.1103/physrevb.79.220514
dc.identifier.issn1550-235X (electronic)
dc.identifier.urihttps://aaltodoc.aalto.fi/handle/123456789/17950
dc.identifier.urnURN:NBN:fi:aalto-201510064535
dc.language.isoenen
dc.publisherAmerican Physical Society (APS)en
dc.relation.ispartofseriesPhysical Review Ben
dc.relation.ispartofseriesVolume 79, Issue 22
dc.rights© 2009 American Physical Society (APS). This is the accepted version of the following article: Kawasaki, S. & Motohashi, T. & Shimada, K. & Ono, T. & Kanno, R. & Karppinen, Maarit & Yamauchi, H. & Zheng, Guo-qing. 2009. Measurement of electron correlations in LixCoO2 (x=0.0-0.35) using 59Co nuclear magnetic resonance and nuclear quadrupole resonance techniques. Physical Review B. Volume 79, Issue 22. 220514/1-4. ISSN 1550-235X (electronic). DOI: 10.1103/physrevb.79.220514, which has been published in final form at http://journals.aps.org/prb/abstract/10.1103/PhysRevB.79.220514.en
dc.rights.holderAmerican Physical Society (APS)
dc.subject.keywordnuclear magnetic resonanceen
dc.subject.keywordnuclear quadrupole resonance techniquesen
dc.subject.keywordsuperconductorsen
dc.subject.keywordelectronic stateen
dc.subject.keywordspin correlationsen
dc.subject.otherChemistryen
dc.subject.otherPhysicsen
dc.titleMeasurement of electron correlations in LixCoO2 (x=0.0–0.35) using 59Co nuclear magnetic resonance and nuclear quadrupole resonance techniquesen
dc.typeA1 Alkuperäisartikkeli tieteellisessä aikakauslehdessäfi
dc.type.dcmitypetexten
dc.type.versionFinal published versionen

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