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dc.contributor.authorKumar, Shalendra-
dc.contributor.authorAlimuddin-
dc.contributor.authorKumar, Ravi-
dc.contributor.authorThakur, P.-
dc.contributor.authorChae, K. H.-
dc.contributor.authorAngadi, Basavaraj-
dc.contributor.authorChoi, Wk-
dc.date.accessioned2024-01-21T00:04:54Z-
dc.date.available2024-01-21T00:04:54Z-
dc.date.created2021-09-02-
dc.date.issued2007-11-28-
dc.identifier.issn0953-8984-
dc.identifier.urihttps://pubs.kist.re.kr/handle/201004/133970-
dc.description.abstractWe present structural, electrical transport, magnetic, and electronic structure studies of Mg(0.95)Mn(0.05)Fe(2-2)xTi(2x)O(4) ferrite using x-ray diffraction, dielectric spectroscopy, DC magnetization and near edge x-ray absorption fine structure (NEXAFS) measurements. The x-ray diffraction study shows a structural transition from cubic to tetragonal with Ti substitution. The dielectric constant and DC conductivity increase with Ti substitution up to x = 0.2. However, with further increase of substitution both the dielectric constant and DC conductivity decrease. This electrical behavior indicates that at low values of substitution, hopping between Fe3+ and Fe2+ increases whereas at higher concentrations the total content of Fe ions decreases. It is observed that all the samples exhibit ferrimagnetic behavior at 300 K and the saturationmagnetization decreases with increase in Ti substitution. The NEXAFS measurements have been carried out at O K-, Fe L-, Fe K-, and Ti L- edges to investigate the chemical states and the electronic structure of the Mg0.95Mn0.05Fe2-2xTi2xO4 ( 0 <= x <= 0.5) system at room temperature. The O K- edge spectra indicate that the Fe 3d orbitals are considerably modified with the substitution of Ti ions. At x >= 0.3, a new spectral feature appears ( similar to 532 eV) due to the transitions from oxygen 2p to Ti 3d orbitals which starts dominating the pre-edge spectra of the system. Both Fe L-3,L-2- and Fe K-edge spectra indicate that iron Fe3+ ions convert into Fe2+ with the substitution of Ti ions. The Ti L-3,L-2- edge NEXAFS spectra reveal that the Ti remains in the 4+ state for all the samples. The observed experimental results have been explained on the basis of dilution of the magnetic sublattice by Ti substitution, which provides a strong interplay between electrical and magnetic properties along with their electronic structure.-
dc.languageEnglish-
dc.publisherIOP PUBLISHING LTD-
dc.subjectDIELECTRIC BEHAVIOR-
dc.subjectZN FERRITES-
dc.subjectMOSSBAUER-
dc.subjectCONDUCTIVITY-
dc.subjectTEMPERATURE-
dc.subjectTRANSITION-
dc.subjectGLASS-
dc.titleElectrical transport, magnetic, and electronic structure studies of Mg(0.95)Mn(0.05)Fe(2-2x)Ti2xO4 +/-delta (0 <= x <= 0.5) ferrites-
dc.typeArticle-
dc.identifier.doi10.1088/0953-8984/19/47/476210-
dc.description.journalClass1-
dc.identifier.bibliographicCitationJOURNAL OF PHYSICS-CONDENSED MATTER, v.19, no.47-
dc.citation.titleJOURNAL OF PHYSICS-CONDENSED MATTER-
dc.citation.volume19-
dc.citation.number47-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.identifier.wosid000250711200013-
dc.identifier.scopusid2-s2.0-36048961790-
dc.relation.journalWebOfScienceCategoryPhysics, Condensed Matter-
dc.relation.journalResearchAreaPhysics-
dc.type.docTypeArticle-
dc.subject.keywordPlusDIELECTRIC BEHAVIOR-
dc.subject.keywordPlusZN FERRITES-
dc.subject.keywordPlusMOSSBAUER-
dc.subject.keywordPlusCONDUCTIVITY-
dc.subject.keywordPlusTEMPERATURE-
dc.subject.keywordPlusTRANSITION-
dc.subject.keywordPlusGLASS-
dc.subject.keywordAuthorelectronic structure-
dc.subject.keywordAuthorNEXAFS-
dc.subject.keywordAuthorFerrite-
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