Structure and magnetic properties of Ni0.64Zn0.36Fe2O4 nanoparticles synthesized by high-energy milling and subsequent heat treatment

High energy ball milling and subsequent annealing were applied to synthesize nanocrystalline Ni 0.64 Zn 0.36 Fe 2 O 4 ferrite from a powder mixture of pure metal Zn, Fe 2 O 3 and NiO in an oxygen atmosphere. The structural and phase evolution of powder particles after different milling times were st...

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Veröffentlicht in:Journal of materials science. Materials in electronics 2015-03, Vol.26 (3), p.1709-1718
Hauptverfasser: Hajalilou, Abdollah, Hashim, Mansor, Mohamed Kamari, Halimah
Format: Artikel
Sprache:eng
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Zusammenfassung:High energy ball milling and subsequent annealing were applied to synthesize nanocrystalline Ni 0.64 Zn 0.36 Fe 2 O 4 ferrite from a powder mixture of pure metal Zn, Fe 2 O 3 and NiO in an oxygen atmosphere. The structural and phase evolution of powder particles after different milling times were studied by X-ray diffractometry. The XRD results showed that a Ni–Zn ferrite was formed with some residual Fe 2 O 3 by annealing a 30-h-milled sample at as low as 400 °C for 2 h. The average crystallite size of the 30 h-milled powder was estimated to be about 15 nm which grew to 21 nm after annealing at 500 °C for 2 h. TEM image showed an agglomerated state of particles for 30 h-milled powders. FT-IR analysis indicated two absorption bands in the Ni–Zn ferrite structure related to octahedral and tetrahedral sites, respectively, in the range of 400–600 cm −1 . Thermogravimetric analysis showed a mass loss about 2 % for as-received powder mixture below 400 °C; after that, it was almost stable. The Ni–Zn ferrite formation mechanism was detected to be in three stages: oxidation of zinc, diffusion of ZnO in Fe 2 O 3 and the formation of ZnFe 2 O 4 , and diffusion of NiO in ZnFe 2 O 4 and the formation of Ni–Zn ferrite. Vibrating sample magnetometery results revealed that a saturation magnetization of the 30 h-milled sample was about 5 emu/g which increased to 16 emu/g after annealing at 400 °C due to a reduction in density of lattice imperfections and strain.
ISSN:0957-4522
1573-482X
DOI:10.1007/s10854-014-2597-4