dc.creatorGoni A.
dc.creatorLezama L.
dc.creatorMoreno N.O.
dc.creatorFournes L.
dc.creatorOlazcuaga R.
dc.creatorBarberis G.E.
dc.creatorRojo T.
dc.date2000
dc.date2015-06-30T19:49:50Z
dc.date2015-11-26T14:46:56Z
dc.date2015-06-30T19:49:50Z
dc.date2015-11-26T14:46:56Z
dc.date.accessioned2018-03-28T21:57:00Z
dc.date.available2018-03-28T21:57:00Z
dc.identifier
dc.identifierChemistry Of Materials. , v. 12, n. 1, p. 62 - 66, 2000.
dc.identifier8974756
dc.identifier10.1021/cm991069c
dc.identifierhttp://www.scopus.com/inward/record.url?eid=2-s2.0-0342409288&partnerID=40&md5=7a5dd0e7b9471657ef52c9600f1e9b0d
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/107151
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/107151
dc.identifier2-s2.0-0342409288
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1253056
dc.descriptionSpectroscopic and magnetic studies on α-Li3Fe2(PO4)3 show an interesting behavior below the transition temperature (29 K). The compound orders antiferromagnetically, presenting a weak ferromagnetic moment, which diminishes with temperature. In the same region of temperatures, the Mossbauer spectra split in two sextets with slightly different hyperfine fields, and the ESR spectrum reduces its intensity and broadens. These results are interpreted as the competition between two sublattices of Fe(III) ions, corresponding to the presence of two independent Fe(III) crystallographic sites in the structure. The magnetic interaction in each sublattice is ferromagnetic, being coupled antiferromagnetically between them. The observed weak ferromagnetic component is the result of the ferrimagnetic character in the coupling between two Fe(III) sublattices.
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dc.languageen
dc.publisher
dc.relationChemistry of Materials
dc.rightsfechado
dc.sourceScopus
dc.titleSpectroscopic And Magnetic Properties Of α-li3fe2(po4)3: A Two-sublattice Ferrimagnet
dc.typeArtículos de revistas


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