Synthesis and characterization of nano-sized pure and Al-doped lithium ferrite having high value of dielectric constant
Introduction
Ferrites form a very good class of electrical materials because of their high resistivity and low loss behaviour, and hence have vast technological applications over a wide range of frequencies [1]. Ferrites assume special significance in the field of electronics and telecommunication industry because of their novel electrical properties which makes them useful in radiofrequency circuits, high quality filters, rod antennas, transformer cores, read/write heads for high digital tapes and other devices [2], [3]. Hence it is important to study their dielectric behaviour at different frequencies. The dielectric properties of ferrites are dependent on several factors, such as method of preparation, heat treatment, sintering conditions, chemical composition, cation distribution and crystallite size [4].
The preparation of ferrites in the nano range had got considerable attention, because the size of the ferrite particles determine whether they are going to behave as super paramagnetic, single domain or multi-domain materials [5]. Many synthesis techniques are available for the nano particle synthesis, however the thermal decomposition of the citrate gel shows good results. This method is simple, does not require high temperature and prolonged heating and gives very fine particles [6]. When a citrate gel is heated on a hot plate, burn itself because of exothermic nature, thus converting the precursor mixture directly into final products. The self-propagating route shows many advantages, like inexpensive, short preparation time, low heating and simplicity. Therefore we have prepared an Al-doped lithium ferrite by this method. Lithium and substituted lithium ferrites are of great importance in the microwave and memory core applications owing to their high Curie temperature, high saturation magnetization, and excellent hysteresis loop properties and less sensitive to stress [7], [8], [9]. In addition lithium ferrites do not contain costly ingredients [10]. Lithium ferrites behave as an n-type semiconductor based on the inverse spinel structure being characterized by high electrical resistivity (105–106 Ω cm) and high Curie temperature (640–680 °C), and are therefore used for gas sensing applications [11].
At low temperature the compound adopts an inverse structure in which the Li+1 and 3/5 of Fe3+ ions occupy B-sites in an ordered fashion, while the remaining Fe3+ ions occupy A-sites and the space group is P4332. At temperature above 735–755 °C, the octahedral B-site occupancy becomes disordered and the solid is indexed according to the space group Fd3m [12]. Synthesis of structurally stabilized lithium ferrite with and without flux is still a hot topic of research in the area of magnetic materials. Several multi-valence atoms can be combined along with lithium to alter properties of the ferrite suitable for a specific use. Substitution with a trivalent cation, to maintain charge neutrality is one of the most important choices. Such mixed lithium ferrites are unique, since they do not contain any divalent cation.
Al3+ substituted lithium ferrites have attracted the attention of several workers. Miles [13], Caster et al. [14], Waxwell and Pickert [15] Schulkes and Blasse [16], Maria et al. [17], Widataulah et al. [8], and George et al. [18] have studied Li–Al ferrites for their electrical and magnetic properties. Jung et al. [19] studied ion distribution in a series of Al3+ doped lithium ferrite. By carefully analyzing the powder X-ray diffractograms, they found that the Al3+ substitute some of the Fe3+ in the tetrahedral as well as octahedral site of the spinel structure. Nanoti et al. [20] studied the electrical and magnetic properties of these ferrites synthesized by ceramic technique. The wider use of lithium ferrites particularly in the microwave devices is restricted because of the difficulties experienced in sintering the material at high temperatures employed to achieve high densities. The high temperature used for sintering (>1000 °C) lead to irreversible loss of lithium and oxygen resulting in a lower saturation magnetization due to the formation of α-Fe2O3 or Fe3O4. Furthermore the reduction of Fe3+ to Fe 2+ due to the formation of Fe3O4 results in an increased conductivity. It is therefore important to try a process not requiring high calcination temperature to induce solid-state reaction.
In the present work we have reported the preparation of Li0.5AlxFe2.5−xO4 (0.0 ≤ x ≤ 0.4) ferrite by citrate gel auto combustion method, in which the pH of the solution was maintained at 6. The powders were characterized by X-ray diffraction (XRD). Electrical properties of the polycrystalline material were studied as a function of frequency and composition at room temperature using dielectric and impedance spectroscopy. The effect of Al3+ substitution on magnetic properties of lithium ferrites have been evaluated by M–H curves at room temperature.
Section snippets
Synthesis
Nano particles of Li0.5AlxFe2.5−xO4 (0.0 ≤ x ≤ 0.4) were prepared by using citrate gel auto combustion method, using analytical grade LiCl (anhydrous), Fe(NO3)3·9H2O and Al(NO3)3·9H2O as starting materials. Metal nitrates taken in the required stoichiometric ratio were dissolved in a minimum amount of distilled water and mixed together. The mixed metal nitrate solution was then added to the citric acid solution in 1:1 molar ratio. The pH value of the clear solution thus obtained value was unity.
X-ray analysis
Fig. 1 shows the X-ray diffraction pattern of lithium ferrite of composition Li0.5AlxFe2.5−xO4 (0.0 ≤ x ≤ 0.4). The XRD data shows that all the compositions exhibit single-phase cubic spinel structure with Fd3m space group and confirms the absence of any secondary phase. The experimental results show that the average crystallite size varies from 38–41 nm. With Al3+ doping the intensity of the central maxima increases and the intensity of the peaks decreases. This is due to the decrease of the
Conclusions
Nano Li0.5Fe2.5−xAlxO4 ferrite was prepared by citrate gel auto combustion method at pH of 6. The average crystallite size is in the range of 38 nm to 41 nm. Lattice parameter, crystallite size and density decreases, with Al doping, which is explained on the basis of ionic radii and density of Al3+ ion. The dielectric properties show the normal behaviour with frequency is explained on the basis of Koop's theory and Maxwell–Wagner model. The ac conductivity first increases up to x = 0.1, then
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