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57Fe hyperfine interaction parameters and selected magnetic properties of high purity MFe12O19 (M=Sr, Ba)

dc.contributor.authorEvans, B. J.en_US
dc.contributor.authorGrandjean, F.en_US
dc.contributor.authorLilot, A. P.en_US
dc.contributor.authorVogel, R. H.en_US
dc.contributor.authorGerard, A.en_US
dc.date.accessioned2006-04-07T19:53:29Z
dc.date.available2006-04-07T19:53:29Z
dc.date.issued1987-05en_US
dc.identifier.citationEvans, B. J., Grandjean, F., Lilot, A. P., Vogel, R. H., Gerard, A. (1987/05)."57Fe hyperfine interaction parameters and selected magnetic properties of high purity MFe12O19 (M=Sr, Ba)." Journal of Magnetism and Magnetic Materials 67(1): 123-129. <http://hdl.handle.net/2027.42/26709>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TJJ-46X4JHV-J5/2/93df295b68e926ccd1b02171c6fc2ed2en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/26709
dc.description.abstractMuch of the confusion regarding the 57Fe Mossbauer spectroscopic hyperfine parameters of SrFe12O19 and BaFe12O19 at 300 K has been removed by means of an interlaboratory investigation of well-characterized samples prepared from high purity starting materials. In contrast to previous investigations, the contributions of each of the five Fe sublattices to the Mossbauer spectrum are discernible at 300 K and five components are necessary for an adequate fit of the data. The relative magnitudes of the hyperfine fields, Hn, and isomer shifts, [delta], are as follows: for SrFe12O19 and BaFe12O19: Hn(2b)Hn(12k)Hn(4f1) Hn(2a)Hn(4f2), for SrFe12O19 [delta](4f12), and for BaFe12O19 [delta]4f2), and for BaFe12O19 [delta](4f11)2)The high purity starting materials seem to have appreciable influences on both hyperfine interaction parameters and bulk magnetic properties as observed by others for spinel and garnet ferrites.en_US
dc.format.extent495320 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.title57Fe hyperfine interaction parameters and selected magnetic properties of high purity MFe12O19 (M=Sr, Ba)en_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelElectrical Engineeringen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, The University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Chemistry, The University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationotherInstitut de Physique, B5, Université de Liège, Sart Tilman, 4000, Liège 1, Belgiumen_US
dc.contributor.affiliationotherInstitut de Physique, B5, Université de Liège, Sart Tilman, 4000, Liège 1, Belgiumen_US
dc.contributor.affiliationotherInstitut de Physique, B5, Université de Liège, Sart Tilman, 4000, Liège 1, Belgiumen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/26709/1/0000259.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0304-8853(87)90728-1en_US
dc.identifier.sourceJournal of Magnetism and Magnetic Materialsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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