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Investigation on X-ray photoelectron spectroscopy, structural and low temperature magnetic properties of Ni-Ti co-substituted M-type strontium hexaferrites prepared by ball milling technique

G.A. Alna'washiDepartment of Physics, The Hashemite University, Zarqa 13115, JordanA. M. AlsmadiDepartment of Physics, Kuwait University, 13060 Safat, KuwaitIbrahim BsoulDepartment of Physics, Al al-Bayt University, Mafraq, JordanB. SalamehDepartment of Physics, Kuwait University, 13060 Safat, KuwaitGassem M. AlzoubiDepartment of Physics, The Hashemite University, Zarqa 13115, JordanM. ShatnawiDepartment of Physics, The Hashemite University, Zarqa 13115, JordanSafeia HamashaDepartment of Physics, The Hashemite University, Zarqa 13115, JordanSami H. MahmoodPhysics Department, The University of Jordan, Amman 11942, Jordan
2021en
ABI

Аннотация

The effect of substituting Fe3+ ions by a combination of divalent Ni2+ and tetravalent Ti4+ in SrM hexaferrites synthesized by mechanical ball-milling technique were reported. Standard SrFe12O19 hexagonal ferrite (P63/mmc) was confirmed by measured XRD patterns. The phase purity was also confirmed by the XPS. The SEM images showed a clear hexagonal-shape particles in the prepared ferrites. The elemental distribution obtained from EDX spectra for SrFe12–2xNixTixO19 (x = 0.2, 0.4, 0.6 and 0.8) was consistent with stoichiometry of the starting powder. X-ray photoelectron spectra confirmed the existence of Fe2+, Fe3+, Ni2+, Ni3+ and Ti4+ ions. The presence of Fe2+ and Ni3+ was correlated with an electron transfer between Fe3+ and Ni2+. By increasing the Ni concentration, we found that some Fe3+ ions are transferred to Fe2+ ions, while some of the Ni2+ ions are transferred to Ni3+ ions. Irreversible ZFC and FC curves were recorded in the 4–300 K temperature range. The isothermal magnetization curves confirmed the ferromagnetic behavior for all synthesized samples. A small variation in the saturation and remnant magnetizations along with a sharp reduction in the coercivity fields with the increase of x were observed in a wide range of temperatures. The broad peak observed in the temperature dependence of the saturation magnetization for x = 0.8 may be referred to the spin reorientation transition. The decrease in the coercivity agrees with the behaviour of the magneto crystalline anisotropy while the first anisotropy constant exhibits a fast decrease above x = 0.6.

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