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dc.contributor.authorHossain, M.D.-
dc.contributor.authorKhan, M.N.I.-
dc.contributor.authorHossain, Md Sarowar-
dc.contributor.authorAhned, S. J.-
dc.contributor.authorAlam, M. K.-
dc.contributor.authorLiba, S. I.-
dc.contributor.authorHakim, M. A.-
dc.contributor.authorJamil, A.T.M.K.-
dc.date.accessioned2025-10-14T09:38:45Z-
dc.date.available2025-10-14T09:38:45Z-
dc.date.issued2022-08-11-
dc.identifier.citationM.D. Hossain, M.N.I. Khan, Md Sarowar Hossain, S.J. Ahned, M.K. Alam, S.I. Liba, M.A. Hakim, A.T.M.K. Jamil, Structure-based magnetic, electrical and transport properties of Ni–Zn–Co ferrite by V5+ substitution, Current Applied Physics, Volume 43, 2022, Pages 36-49, https://doi.org/10.1016/j.cap.2022.05.012.en_US
dc.identifier.issn1567-1739-
dc.identifier.urihttps://www.sciencedirect.com/science/article/pii/S1567173922001213-
dc.identifier.urihttp://dspace.aiub.edu:8080/jspui/handle/123456789/2906-
dc.description.abstractThis article presents the modification of structure-based magnetic, electronic and transport properties along with the conduction mechanism and its relaxation process in a Ni–Zn–Co ferrite tailored by V5+substitution at B-site replacing Fe3+ions. The composition Ni0.7Zn0.2Co0.1Fe2-xVxO4 (0≤x≤0.12) was synthesized by standard solid- state reaction method and all samples were crystallized with a single-phase cubic spinel structure belonging to the Fd3m space group. The lattice constants decreased gradually from 8.3673 Å to 8.3602 Å and the average grain sizes (DSEM)are also decreased from 6.92 μm to 1.99 μm due to V5+ ions substitution at Fe3+ of B-site. However, more than 25% of Fe3+ ions migrate to A-site from B-site due to V5+ substitution at Fe3+of B-site. In all samples θD does not strictly follow the Anderson’s prediction, rather it monotonically decreases to a low value until x= 0.12. Magnetic phase transition temperature shifted to the lower temperature and the net magnetization (n_B^e ) decreases due to V5+ substitution in Ni–Zn–Co ferrite. Apart this, during conduction charge carriers should require more energy to jump from one cationic site to other for V5+ substitution in the Ni–Zn–Co ferrite and the activation energy (Ea) is much more higher in V5+ substituted sample. Moreover, long-range interaction with localized relaxation mechanism is observed in V5+ doped samples. The resistance at the grain (Rg) is maximum (243.09 Ω) for the sample x=0.10 while grain boundary resistance (Rgb) is maximum (5.98×105 Ω) for the sample x=0.07. However, the higher value of ρ_DC for x=0.12 sample ensures to be suitable for electromagnets, transformers, electronic inductors, and at high-frequency applications. Moreover, x=0.07 sample displays high value of TCR (8.6 %/K at 418 K) which may be utilized as an infrared detector for night vision bolometer material.en_US
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.subjectCation distributionen_US
dc.subjectThermo-magnetizationen_US
dc.subjectDebye temperatureen_US
dc.subjectPhase angleen_US
dc.subjectRelaxation mechanismen_US
dc.subjectTransport propertiesen_US
dc.titleStructure-based magnetic, electrical and transport properties of Ni–Zn–Co ferrite by V5+ substitutionen_US
dc.typeArticleen_US
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