Full metadata record
DC Field | Value | Language |
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dc.contributor.author | Kumar, Shalendra | - |
dc.contributor.author | Alimuddin | - |
dc.contributor.author | Kumar, Ravi | - |
dc.contributor.author | Thakur, P. | - |
dc.contributor.author | Chae, K. H. | - |
dc.contributor.author | Angadi, Basavaraj | - |
dc.contributor.author | Choi, Wk | - |
dc.date.accessioned | 2024-01-21T00:04:54Z | - |
dc.date.available | 2024-01-21T00:04:54Z | - |
dc.date.created | 2021-09-02 | - |
dc.date.issued | 2007-11-28 | - |
dc.identifier.issn | 0953-8984 | - |
dc.identifier.uri | https://pubs.kist.re.kr/handle/201004/133970 | - |
dc.description.abstract | We 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.language | English | - |
dc.publisher | IOP PUBLISHING LTD | - |
dc.subject | DIELECTRIC BEHAVIOR | - |
dc.subject | ZN FERRITES | - |
dc.subject | MOSSBAUER | - |
dc.subject | CONDUCTIVITY | - |
dc.subject | TEMPERATURE | - |
dc.subject | TRANSITION | - |
dc.subject | GLASS | - |
dc.title | Electrical transport, magnetic, and electronic structure studies of Mg(0.95)Mn(0.05)Fe(2-2x)Ti2xO4 +/-delta (0 <= x <= 0.5) ferrites | - |
dc.type | Article | - |
dc.identifier.doi | 10.1088/0953-8984/19/47/476210 | - |
dc.description.journalClass | 1 | - |
dc.identifier.bibliographicCitation | JOURNAL OF PHYSICS-CONDENSED MATTER, v.19, no.47 | - |
dc.citation.title | JOURNAL OF PHYSICS-CONDENSED MATTER | - |
dc.citation.volume | 19 | - |
dc.citation.number | 47 | - |
dc.description.journalRegisteredClass | scie | - |
dc.description.journalRegisteredClass | scopus | - |
dc.identifier.wosid | 000250711200013 | - |
dc.identifier.scopusid | 2-s2.0-36048961790 | - |
dc.relation.journalWebOfScienceCategory | Physics, Condensed Matter | - |
dc.relation.journalResearchArea | Physics | - |
dc.type.docType | Article | - |
dc.subject.keywordPlus | DIELECTRIC BEHAVIOR | - |
dc.subject.keywordPlus | ZN FERRITES | - |
dc.subject.keywordPlus | MOSSBAUER | - |
dc.subject.keywordPlus | CONDUCTIVITY | - |
dc.subject.keywordPlus | TEMPERATURE | - |
dc.subject.keywordPlus | TRANSITION | - |
dc.subject.keywordPlus | GLASS | - |
dc.subject.keywordAuthor | electronic structure | - |
dc.subject.keywordAuthor | NEXAFS | - |
dc.subject.keywordAuthor | Ferrite | - |
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