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Structure, impedance spectroscopy, and magnetic properties of nanostructured composites (1-x)CoFe2O4–xPbTiO3

Bashir AbdulvakhidovDagestan State University, Gadgieva 43a, Makhachkala, 367000, RussiaS. A. SadykovDagestan State University, Gadgieva 43a, Makhachkala, 367000, RussiaК. Г. АбдулвахидовSouthern Federal University, Sladkova 178/24, Rostov-on-Don, 344090, RussiaAlexander SoldatovSouthern Federal University, Sladkova 178/24, Rostov-on-Don, 344090, RussiaZhengyou LiSouthern Federal University, Sladkova 178/24, Rostov-on-Don, 344090, RussiaYury V. RusalevSouthern Federal University, Sladkova 178/24, Rostov-on-Don, 344090, RussiaА. В. НазаренкоSouthern Scientific Center of the Russian Academy of Sciences, Chekhova 41, Rostov-on-Don, 344006, RussiaPavel PlyakaSouthern Scientific Center of the Russian Academy of Sciences, Chekhova 41, Rostov-on-Don, 344006, RussiaSalim OtajonovFergana State University, Murabbiylar 19, Fergana, 100150, UzbekistanNurzod YunusovFergana State University, Murabbiylar 19, Fergana, 100150, UzbekistanMaхamatjon AxmеdovFergana State University, Murabbiylar 19, Fergana, 100150, UzbekistanM. A. VitchenkoDon State Technical University, Gagarina 1, Rostov-on-Don, 344000, RussiaI. V. MardasovaDon State Technical University, Gagarina 1, Rostov-on-Don, 344000, Russia
Ceramics Internationaljournal2024en
ABI

Аннотация

The article presents a comprehensive investigation of the crystal structure, impedance spectra, magnetic, magnetodielectric, and magnetoresistive properties of (1- x )CoFe 2 O 4 – x PbTiO 3 composites with varying concentrations ( х = 0, 0.2, 0.4, and 0.6). The study also examines the effects of applying a uniaxial pressure of 1 GPa to the synthesized powders using Bridgman anvils. Our findings reveal that the synthesis of these composites results in the formation of an additional phase, lead hexaferrite PbFe 12 O 19 , which exhibits multiferroic properties. Additionally, the coherent scattering region of the components is significantly reduced after mechanical activation . Notably, the real part of the resistivity ρ ′( ω ) of nanostructured CoFe 2 O 4 ceramics increases eightfold at T = 240 °C. The composites demonstrate significant magnetoresistance at room temperature, reaching up to 250 %. The study also reveals that the signs of the magnetodielectric MD ( B ) and magnetoresistive coefficient MR ( B ) vary with the frequency of the measuring field for certain concentrations. Using the first-order reversal curve (FORC) method, it was observed that after nanostructuring CoFe 2 O 4 through mechanical activation, the interaction field H u shifts from ± 0.6 kOe to ± 0.8 kOe, while the coercive field H c increases from 1.05 kOe to 5 kOe. Moreover, the two-dimensional FORC maps of the composites show increased complexity, due to the formation of additional magnetic phases.

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