Structural analysis, magnetic and electrical properties of samarium substituted lithium–nickel mixed ferrites
Highlights
▸ A-site radii increased and B-site radii decreased with Sm content increase. ▸ Sm doping increased the resistivity due to the decrease in charge mobility. ▸ High dielectric constant achieved due to the rise in hopping between Fe2+ and Fe3+. ▸ Samples magnetization under applied field exhibited a clear hysteretic behavior. ▸ MS increased with the sintering temperature, while HCi was found to decrease.
Introduction
Lithium ferrites are low cost materials and have important magnetic and electrical properties for the applications of microwave devices, such as isolators, circulators and phase shifters. It is known that the intrinsic parameters of ferrites, such as magnetization, low dielectric losses, Curie temperature and resistivity, depend on the chemical composition, heat treatment and type of additive or substituted ions. In addition, the rectangularity of B–H loop is also found to increase with increasing defects that hinder the magnetic domain wall motion within the grains [1]. It is interesting to note that the electromagnetic properties of spinel ferrites can be tailored by controlling the type and amount of transition metallic substitutes. Until now, several investigations have been carried on to make further improvements in the electric, dielectric and magnetic properties of substituted lithium ferrites. The rare earth oxides are becoming promising additives for the improvement of ferrite properties. It is known that rare earth (RE) ions have unpaired 4f electrons, which have the role of originating magnetic anisotropy because of their orbital shape. The magnetocrystalline anisotropy in ferrite is related to the 4f–3d couplings between the transition metal and rare earth ions; thus doping rare earth ions into spinel lithium ferrite can improve their electrical and magnetic properties. Many researchers have studied the influence of various rare earth doping atoms on the properties of, Li–Ni, Ni–Zn, Mn–Zn, Mg–Cu, Cu–Zn ferrites, etc. [2], [3], [4], [5], [6]. The results of these researches show that different rare-earth ions behave differently in spinel ferrite. In general, the permeability of ferrite (e.g. Ni–Zn) was reported to decrease with the substitution of R2O3. An increase of about 60% relative permeability in Sm-doped Cu–Zn ferrite is reported by Sattar et al. [1]. Jalli et al. [7] report on the Samarium (Sm) doped M-type strontium ferrite single crystals. Dwevedi et al. [8] report on the structural, electrical and magnetoreactance of Dy, Gd and Nd-doped Ni ferrites. Some literature reports the decrease in relative density of ferrites with rare earth addition. On the other hand, others report on its increase. It has been accepted that the rare-earth ions commonly reside at octahedral sites and have limited solubility in the spinel lattice due to their large ionic radii. Nevertheless, the precise value of their solubility in the spinel lattice is not well known [9], [10].
In the present work, the magnetic, electric and dielectric properties of Sm-substituted Li–Ni spinel ferrite are synthesized and characterized as a function of composition, frequency and sintering temperature. This may provide interesting properties due to the cations redistribution in the tetrahedral A and octahedral B—sites of the spinel structure. Both mechanisms of dielectric polarization and domain walls motion are discussed in detail in this work.
Section snippets
Experimental
Polycrystalline Sm-substituted Li–Ni ferrites, having the chemical formula (Li0.5Fe0.5)0.4Ni0.6SmyFe2−yO4 (where 0≤y≤0.1), were prepared by double sintering ceramic technique. Analytical grade materials: Sm2O3, Fe2O3, NiCO3·2Ni(OH)2·4H2O and Li2CO3 were mixed in the proper ratio to give stoichiometric compound. The mixed powders were pre-sintered at 900 °C for 3 h in air, and then remixed to increase the homogeneity. Samples in the shape of pellets (diameter=15 mm and thickness ≈2 mm) were prepared
Results and discussion
Fig. 1 shows the XRD patterns of the samples with different doping levels of Sm3+ ions. The characteristic peaks belong to the (Fd3m) cubic spinel space group. It indicates the formation of the single-phase spinel ferrite structure. A crystalline secondary phase, identified as garnet (Sm3Fe5Ol2) or orthoferrite (SmFeO3), in a small amount existed. The secondary phases formed on the grain boundaries resulted from the following reactions:3Sm2O3+5Fe2O3=2Sm3Fe5Ol2 and5Fe2O3+5 Sm2O3=10SmFe O3and
Conclusion
Summarizing the experimental results for the studied ferrite (Li0.5Fe0.5)0.4Ni0.6SmyFe2−y O4, the following points are concluded: (1) the decrease in LA shows no effect on the resistivity, which confirms the preference of Ni2+ for the B-site according to the suggested conductivity mechanism. (2) Sm doping increases the resistivity through the increase in B-site hopping length LB leading to decrease in charge mobility. (3) There is a strong correlation between the conduction mechanism and the
Acknowledgment
The authors would like to acknowledge with gratitude the help from the School of Materials Science and Engineering-University of New South Wales-Australia for the support to finish this work. Two of the authors (Muthafar Al-Hilli and Kassim S. Kassim) are grateful to the University of Baghdad and University of Technology for support.
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