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hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCASTETS, Aurore
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCARLIER-LARREGARAY, Dany
hal.structure.identifierInstitut des Matériaux Jean Rouxel [IMN]
dc.contributor.authorZHANG, Yuesheng
hal.structure.identifierInstitut des Matériaux Jean Rouxel [IMN]
dc.contributor.authorBOUCHER, Florent
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorMARX, Nicolas
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCROGUENNEC, Laurence
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorMÉNÉTRIER, Michel
dc.date.issued2011
dc.identifier.issn1932-7447
dc.description.abstractEn<sup>7</sup>Li, <sup>31</sup>P, and <sup>1</sup>H MAS NMR spectra and magnetic properties are reported for LiFePO<sub>4</sub>*OH and FePO<sub>4</sub>*H<sub>2</sub>O. The former shows no Curie-Weiss-type behavior up to room temperature, while the latter tends to such a behavior in a restricted temperature range. Calculation strategies are discussed for the NMR shifts that result from Fermi contact interaction with the high spin Fe<sup>3+</sup> ions. Zero Kelvin electron spin densities obtained by averaging over the ion size using VASP (with PAW potentials) range with those obtained at the nucleus from WIEN2k, with the GGA and GGA+U methods. The latter values have been scaled with the temperature of the NMR measurement by using the experimental magnetic susceptibility, yielding calculated NMR shifts. The agreement is quite satisfactory, but very much dependent on the exchange correlation potential used for the calculation. Possible reasons for this are discussed, also considering the difference in magnetic behaviors.
dc.language.isoen
dc.publisherAmerican Chemical Society
dc.title.enMultinuclear NMR and DFT calculations on the LiFePO<sub>4</sub>.OH and FePO<sub>4</sub>.H<sub>2</sub>O homeotypic phases
dc.typeArticle de revue
dc.identifier.doi10.1021/jp204767c
dc.subject.halChimie/Matériaux
bordeaux.journalJournal of Physical Chemistry C
bordeaux.page16234-16241
bordeaux.volume115
bordeaux.issue32
bordeaux.peerReviewedoui
hal.identifierhal-00619811
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00619811v1
bordeaux.COinSctx_ver=Z39.88-2004&amp;rft_val_fmt=info:ofi/fmt:kev:mtx:journal&amp;rft.jtitle=Journal%20of%20Physical%20Chemistry%20C&amp;rft.date=2011&amp;rft.volume=115&amp;rft.issue=32&amp;rft.spage=16234-16241&amp;rft.epage=16234-16241&amp;rft.eissn=1932-7447&amp;rft.issn=1932-7447&amp;rft.au=CASTETS,%20Aurore&amp;CARLIER-LARREGARAY,%20Dany&amp;ZHANG,%20Yuesheng&amp;BOUCHER,%20Florent&amp;MARX,%20Nicolas&amp;rft.genre=article


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