Cation distribution and magnetic properties of CoAlxFe2−xO4/SiO2 nanocomposites
Introduction
Cubic spinel ferrite, crystallizing with space group Fd3m, has two sublattices, tetrahedral (A) sites and octahedral (B) sites. The important structural, electrical and magnetic properties of spinels, responsible for their application in various fields, are found to depend on the distribution of cations among sites. Therefore the estimation of cation distribution turns out to be important [1], [2], [3]. In addition, in order to understand the magnetic interaction behavior, it is necessary to perform non-magnetic cation (Al3+, Y3+) doping [4], [5]. But when Al3+ substitutes for Fe3+ in CoFe2O4 ferrite, the problem of the distribution of Al3+ between A- and B-sites is often been oversimplified in the literatures. Thanki et al. regarded Al3+ to only occupy B-site for ZnxCo1−xAlxFe2−xO4 [6]. Singhal et al. guessed that Al3+ entered into the A- and B-sites in the ∼2:3 ratio for CoAlxFe2−xO4 [7]. Mane et al. [8] and More et al. [9] obtained the ratio as 1:4 for CoAlxCrxFe2−2xO4. The reason for the oversimplification is that they only employed the X-ray diffraction to obtain cation distribution. It is well known that the intensities of (2 2 0), (2 2 2), (4 2 2) and (5 1 1) reflections of ferrite are mostly sensitive to cation distribution [10]. It is proposed to use the X-ray diffraction to investigate cation distribution of ZnFe2O4, MgFe2O4 and CuFe2O4. But for CoFe2O4 ferrite, it is difficult to do for the atomic number of Co being approximate to Fe. The Mössbauer technique is known to be a useful tool for investigation of the distribution of Fe3+ in A- and B-sites for ferrite.
In this paper, we study the structural and magnetic properties of CoAlxFe2−xO4/SiO2 (x=0.0–1.0) nanocomposites by X-ray diffraction (XRD), transmission electron microscope (TEM), Mössbauer spectroscopy (MS) and vibrating sample magnetometer (VSM). The main purpose is to obtain cation distribution of CoAlxFe2−xO4/SiO2 nanocomposites by combining the results of MS and XRD. MS is to study the distribution of Fe3+ and XRD is to investigate the assignation of Co2+ and Al3+.
Section snippets
Experiments
CoAlxFe2−xO4/SiO2 (x=0–1.0) nanocomposites were prepared by the sol–gel method using a precursor solution obtained from the mixture of Co(NO3)2·6H2O, Fe(NO3)3·9H2O, Al(NO3)3·9H2O, tetraethylorthosilicate (TEOS), methoxyethanol, glycol, glacial acetic acid and deionized water. The mass ratio of CoAlxFe2O4 and SiO2 was 7:3. The mixtures were magnetically stirred for 5 h. Black brown sols were obtained after complete dissolution, which were evaporated on a water bath at 60 °C to remove the excess
Results and discussion
Fig. 1 shows the XRD patterns of the samples. It can be seen that there are only the diffraction peaks for cubic spinel ferrite. The SiO2 matrix should remain amorphous in the samples. With increasing Al content x, the diffraction peaks became broader and shifted to a higher 2θ position, indicating the decrease in grain size and lattice constant for CoAlxFe2O4 in the nanocomposites. Table 1 shows the values of lattice constant, average grain size, and X-ray intensity ratios of the samples. The
Conclusion
CoAlxFe2−xO4/SiO2 (x=0.0–1.0) nanocomposites have been prepared successfully by the sol–gel method. The cations distribution is determined combining the results obtained by fitting the Mössbauer spectra and the integrated intensity of XRD peaks. The results indicate that Al3+ besides preferring B-site, have also a small tendency to occupy A-site. The ratio of Al3+(B)/Al3+(A) increases with increasing x, which indicates that the preference of Al3+ to occupy B-site increases with increasing Al
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