dc.creatorNowik, I
dc.creatorFelner, I
dc.creatorAwana, VPS
dc.date1999
dc.dateFEB
dc.date2014-12-02T16:29:05Z
dc.date2015-11-26T16:46:21Z
dc.date2014-12-02T16:29:05Z
dc.date2015-11-26T16:46:21Z
dc.date.accessioned2018-03-28T23:32:10Z
dc.date.available2018-03-28T23:32:10Z
dc.identifierJournal Of Magnetism And Magnetic Materials. Elsevier Science Bv, v. 192, n. 1, n. 67, n. 72, 1999.
dc.identifier0304-8853
dc.identifierWOS:000078289900009
dc.identifier10.1016/S0304-8853(98)00383-7
dc.identifierhttp://www.repositorio.unicamp.br/jspui/handle/REPOSIP/82402
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/82402
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/82402
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1274494
dc.descriptionThe compound PrSr2Fe3O9-delta (delta(similar to) < 0.1) has been studied by magnetization and Fe-57 Mossbauer spectroscopy measurements, The magnetization studies show magnetic hysteresis phenomena at low temperatures and three distinct phase transitions: an antiferromagnetic transition at T-N = 190 K, a transition at T-v = 170 K associated with change in iron valence and T-irr = 270 K, the merging temperature of the zero field and field cooled magnetization curves. Mossbauer studies confirm the T-N and T-v values. Well below and above T-N, the spectra are composed of two well-defined sub-spectra (ratio 2 : 1), though all Fe ions reside in one crystallographic site. At 4.2 K the subspectra differ in their isomer shift (IS) by 0.4 mm/s and in the magnetic hyperfine field (469 and 269 kOe) whereas above T-N the difference in the IS is only 0.24 mm/s. For 90 K < T < T-N the spectra ape complex: and cannot be interpreted in terms of well defined (2 or even 3) sub-spectra. All spectra, in the entire temperature range can be well explained and reproduced by a triple valence fluctuation model, assuming that Fe appear in three valence stares. (a) 2Fe(3+) + Fe5+ at low temperatures, (b) Fe3+ and 2Fe(4+) above T-N and (c) at 90 K < T < T-N triple valence fluctuations occur: Fe3+ <-> Fe5+ <-> Fe5+. An electron is transferred from Fe3+ to Fe5+ to form two nonmagnetic Fe4+ ions, This process dilutes the magnetic ions concentration to a point of collapse of the magnetic order. (C) 1999 Elsevier Science B.V. All rights reserved.
dc.description192
dc.description1
dc.description67
dc.description72
dc.languageen
dc.publisherElsevier Science Bv
dc.publisherAmsterdam
dc.publisherHolanda
dc.relationJournal Of Magnetism And Magnetic Materials
dc.relationJ. Magn. Magn. Mater.
dc.rightsfechado
dc.rightshttp://www.elsevier.com/about/open-access/open-access-policies/article-posting-policy
dc.sourceWeb of Science
dc.subjectphase transitions
dc.subjectvalence fluctuations
dc.subjectcanted antiferromagnetism
dc.subjectMossbauer spectroscopy
dc.subjectirreversibility
dc.subjectmagnetic hysteresis
dc.subjectNonstoichiometric Perovskite Sr2lafe3o8+y
dc.subjectMossbauer-spectroscopy
dc.subjectCharge Disproportionation
dc.subjectOxygen Vacancies
dc.titleMagnetic properties and triple valence fluctuations of iron in PrSr2Fe3O9-delta
dc.typeArtículos de revistas


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