Synthesis and Characterization of Cobalt Ferrite (Cofe 2. ) Nanoparticles by Sol-Gel Autocombustion Method
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1 Invertis Journal of Science H.B. and Sharma, Technology, N.G. Boinis Vol. Singh, 7, No. S. 2, Bobby Singh ; pp. and Th. Dhanabati Devi Synthesis and Characterization of Cobalt Ferrite (Cofe 2 ) Nanoparticles by Sol-Gel Autocombustion Method H.B. SHARMA, N.G. BOINIS SINGH, S. BOBBY SINGH* and TH. DHANABATI DEVI Department of Physics, Manipur University, Canchipur * sbsoram@gmail.com Abstract Cobalt ferrite were synthesized by the sol-gel autocombustion method. To modify the features of the particles according to different requirements, the molar ratio of the metal nitrates to citric acid were varied. The final products obtained with different starting conditions were characterized through X-ray diffraction, Scanning Electron Microscopy and Energy Dispersive X-ray. Dielectric and magnetic measurements were finally carried out and the connection between structural and magnetic properties will be discussed. Key words : Nanoparticle, ferrite, sol-gel, dielectric, magnetic. 1. Introduction In recent years, nanocrystalline materials are becoming a subject of intense research because of their unique properties, both from the fundamental and application point of view [1]. Among the ferrites, the most popular type is the cubic spinel structure, which has tetrahedral [A] site and octahedral [B] site in the AB 2 crystal structure [2]. Due to the large electronegativity of oxygen, the ionic type of bonds prevails in almost all oxide spinels [3]. Soft spinel ferrite (MFe 2, Ni, Zn, Mn, etc.) have been intensively investigated due to their remarkable magnetic and electrical properties and wide practical applications in ferrofluids, magnetic drug delivery, magnetic highdensity information storage [4-6]. Hard spinel ferrites, CoFe 2 is an interesting magnetic material because of its high coercivity, moderate saturation magnetization, excellent chemical stability and mechanical hardness. The properties of ferrite are influenced by the composition and microstructure, which are sensitive to the preparation methodology used in their synthesis. There are several different synthesis methods used to generate ferrites such as sol-gel [7], co- precipitation [8], hydrothermal [9], etc. Recently, a sol-gel auto-combustion method has attracted much attention due to its inherent advantages of low processing temperature, homogeneous reactant distribution, the products obtained by this method exhibit high crystalline quality, narrow size distribution and uniform shape [10]. It has been reported that in chemical solution method ph has strong effect on the properties of ferrite. Herein, we reported a simple sol gel auto-combustion method to synthesize nanocrystalline cobalt ferrite. The structural, dielectric and magnetic properties of nanocrystalline cobalt ferrites in relation to the metal nitrate to citric acid ratios were investigated. 2. Experimental Nanocrystalline cobalt ferrite were prepared by sol gel auto-combustion method, using the analytically pure grade [Fe(NO 3 ) 3.9H 2 O], [Co(NO 3 ) 2 6H 2 O], and citric acid (C 6 H 8 O 7 ). Citric acid is used as a fuel. A stoichiometric amount of metal nitrates were dissolved in a certain amount of deionized water by stirring on a hotplate at 50 o C. Citric acid was then added to the mixture solution 78
2 Synthesis and Characterization of Cobalt Ferrite (Cofe 2 ) Nanoparticles by Sol-Gel Autocombustion Method to chelate metal ions. Four samples of different molar ratios of metal nitrate to citric acid such as 3:1, 3:2, 3:3 and 3:4 were prepared. These four samples will be named as CFO1, CFO2, CFO3 and CFO4 respectively hereafter. The ph of the corresponding solutions thus obtained resulted <1. The dark brown solutions were allowed to evaporate on a hot plate maintaining the solution temperature at C. As a result of the increasing concentration, a gel started to form. A sudden increase of the temperature (T>200 C) allowed to convert directly the gels into the corresponding nanocrystalline CoFe 2 powders. The as-prepared powders were then calcined at 400 o C for 4 hrs in free atmosphere. X-ray diffraction (XRD) patterns of the samples were collected on a Philips X'pert Pro X-ray diffractometer. SEM images and EDAX were carried out on a FEI QUANTA 250 scanning electron microscope. Magnetic measurements were carried out at room temperature using a vibrating sample magnetometer (VSM). 3. Results and Discussion 3.1 X-ray Diffraction Analysis Figure 1 shows the X-ray diffraction patterns of the four CFO samples calcined at 400 o C for 4hrs in free atmosphere. These patterns confirm the formation of cubic spinel type lattice of CoFe 2, which matches well with the standard XRD pattern (ICDD card No: ). All peaks correspond to a cubic spinel type lattice (space group Fd3m). It is observed from Fig. 1, that with increase in molar amount of the citric acid the corresponding XRD peaks shifts towards the lower angle suggesting an increase in lattice parameter. The lattice parameter a=b=c of the unit cell were evaluated from the XRD pattern and found to increase from 8.33 to 8.36 Å approaching to that of standard value (8.39Å) of bulk CFO sample [11], with the increase in citric acid amount the crystallite size increases. The average crystallite size of the CFO samples were Intensity (arb.units) (220) (222) (440) (511) (442) (440) (311) θ (Degrees) Fig. 1. X-ray diffraction pattern of CoFe 2 samples calcined at 400 C for 4 hrs Table 1 Structural and dielectric properties of CoFe 2 CoFe 2 a Crystallite size Grain size Dielectric Dissipation Sample (nm) (nm) from (nm) from constant (ε ) factor (D) XRD SEM at 100 khz at 100 khz CFO CFO CFO CFO
3 H.B. Sharma, N.G. Boinis Singh, S. Bobby Singh and Th. Dhanabati Devi determined from the full width at half maximum (FWHM) of the major peak, in Fig. 1 using the Scherrer's formula and are reported in Table 1. The crystallite sizes of the samples were found to increase from 27 nm to 72 nm with the increase in molar amount of citric acid. 3.2 Morphological Behavior of CoFe 2 The structural morphology of was investigated through SEM. Figure 2 shows the SEM images of CoFe 2. The SEM images are also present in the images. The average grain size was found to increase from 42 nm to 95 nm with increase in mole amount of citric acid present. From the morphology it is interesting to note that when citric acid amount content increases the shape does not change but affects only the radius of the EDAX spectrum Figure 3 shows the EDAX spectra of the CFO1 sample and confirmed the ratio of the transition Fig. 2. SEM photograph of four different CoFe 2 show that the CoFe 2 prepared by sol-gel auto-combustion method have uniform spherical structure morphology with a narrow size distribution of particles. Some moderately agglomerated particles as well as separated particles metal atoms in each material according to the nominal stoichiometry. The atomic ratio of Fe:Co for the entire sample (Fig. 3) is maintained at ~ 2:1. These results revealed the sustained spinel structure of the CoFe 2 crystal at low calcinations temperature. 80
4 Synthesis and Characterization of Cobalt Ferrite (Cofe 2 ) Nanoparticles by Sol-Gel Autocombustion Method Label A: CFOSC C:/edax32\genesis\genspc.spc FeK 0K FeL CoK FeK FeL CoK KeV Energy (KeV) Fig. 3. EDAX line scanning spectrum of sample CFO1 nanopowder 3.3 Dielectric Properties Figure 4 (a) and (b) displays the variation of dielectric constant and dissipation factor for four CFO samples as a function of frequency at room temperature from 1k Hz-1MHz. It has been reported that the materials having high d.c. electrical resistivity acquires low values of dielectric constant and vice versa [12]. It is also reported that the polarization in ferrites is mainly contributed by the space charge polarization, which is governed by the number of space charge carriers and the conductivity in materials [13] and hopping exchange of the charges between two localized states governed by density of the localized state and resultant displacement of charges w.r.t. the external field. So, the decrease in dielectric constant with increasing frequency may be attributed to the two factors that (i) the electron exchange between Fe 2+ and Fe 3+ ions cannot follow the change of the external applied field beyond certain frequency [14] and (ii) the dipoles due to the space-charge polarization or Maxwell-Wagner type interfacial polarization do not respond at higher frequencies. It is observed from the figure that the room temperature dielectric constant increases from 104 to 354 with increase in citric acid amount content. The increase in dielectric constant in our sample might me be due to the increase in grain size as suggested by XRD and SEM. Figure 4(b) shows the variation of dissipation factor of CFO samples as a function of frequency at room temperature from 1 khz-1mhz. The dielectric loss factor is considered to be the most important part of the total core loss in ferrites [15, 16]. All the samples show low dielectric loss of ~0.05 at 100 khz. The dielectric loss originates from two mechanisms: resistive loss and relaxation loss. 3.4 Magnetic Properties of the Products The magnetic properties of the CoFe 2 was measured through vibrating sample magnetometer (VSM) at a maximum applied field of 22,000 Oe at room temperature and is shown in Fig. 5. The saturation magnetization (Ms), remanent magnetization (Mr) and coercive field (Hc) of the sample were found to be 38 emu/g,
5 H.B. Sharma, N.G. Boinis Singh, S. Bobby Singh and Th. Dhanabati Devi (b) Frequency (Fig. a) Frequency (khz) (Fig. b) Fig. 4. Variation of room temperature (a) dielectric constant and (b) loss tangent as a function of frequency for CoFe 2 82
6 Synthesis and Characterization of Cobalt Ferrite (Cofe 2 ) Nanoparticles by Sol-Gel Autocombustion Method CFO1 40 Magnetization (emu/gm) K -12.0K -6.0K K 12.0K 18.0K Applied magnetic field (Oe) Fig. 5. Room temperature magnetic hysteresis loop of CoFe 2 emu/g and 1500 Oe, respectively. This value of saturation magnetization is much lower than the bulk value of 80 emu/g [23]. The high coercivity value in our sample indicates that the particles formed are indeed single domain with no nonmagnetic impurities. It is very well reported in literature that the magnetic properties of nanosize particles depend on the preparation method and the particle size. The lower value of saturation magnetization and higher value of coercivety in our sample might be due to smaller grain size. 4. Conclusion Spinel CoFe 2 ferrite system was successfully prepared by Sol-gel autocombustion technique with nano-size dimension. The XRD revealed that the prepared samples possess single phase cubic spinel structure. The nanocrystalline nature of the prepared samples was also confirmed from SEM. The EDAX confirmed the ratio of the transition metal atoms in each material according to the nominal stoichiometry. It is also observed that the dielectric constant increases with increase in the molar ratio of metal nitrate to citric acid amount. The saturation magnetization (M s ), remanent magnetization (M r ) and coercive field (H c ) of the sample were found to be 38 emu/g, emu/g and 1500 Oe, respectively. Acknowledgement One of the authors, Th. Dhanabati Devi is thankful to the UGC, New Delhi, for providing financial assistance as project fellow. References [1] P. Dutta, M.S. Seehra, S. Thota and J. Kumar, J. Phys. Condens. Matter, 20 (2008) [2] C.S. Kim, S.W. Lee, S.L. Park, J.Y. Park and Y.J. Park, J. Appl. Phys., 79 (1996) [3] E.P. Wohlfarth, Ferromagnetic Materials, 3, North-Holland, Amsterdam, (1982). [4] M.P. Pileni, Adv. Funct. Mater., 5 (2001) 323. [5] F.Y. Cheng, C.H. Su, Y.S. Yang, C.S. Yeh, C.Y. Tsai, C.L. Wu, M.T. Wu and D.B. Shieh, Biomaterials, 26 (2005) 729. [6] Q. Song and Z.J. Zhang, J. Am. Chem. Soc., 126 (2004) [7] A. Pradeep, P. Priyadharsini and G. 83
7 H.B. Sharma, N.G. Boinis Singh, S. Bobby Singh and Th. Dhanabati Devi Chandrasekaran, J. Magn. Magn. Mater., 320 (2008) [8] S.G. Doh, E.B. Kim, B.H. Lee and J.H. Oh, J. Magn. Magn. Mater., 2238 (2004) 272. [9] B. Baruwati, R.K. Rana and S.V. Manorama, J. Appl. Phys., 101 (2007) [10] C.J. Brinker and G.W. Scherer, Sol-Gel Science, Academic Press, Boston, (1990). [11] E. Tirosh, G. Shemer and G. Markovich, Chem. Mater., 18 (2006) 465. [12] T. Kanai, S. Ohkoshi and K. Hashimoto, J. Phys. Chem. Solid., 64 (2003) 391. [13] L. Mytil Kahn and Z. John Zhang, Appl. Phys. Lett., 78 (2001) 365. [14] A. M. Abo El Ata, S. M. Attia and T. M. Meaz, Solid State Sci., 6 (2004) 61. [15] F.G. Brockman, P.H. Dowling and W.G. Steneck, Phys. Rev., 75 (1949) [16] R.V. Mangalaraja, S. Ananthakumar, P. Manohar and F.D. Gnanam, J. Magn. Magn. Mater., 253 (2002) 56. [17] L.D. Tung, V. Kolesnichenko, D. Caruntu, N.H. Chou, C.J. O'Connor and L. Spinu, J. Appl. Phys., 93 (2003)
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