Next Article in Journal
Injury Biomechanics Evaluation of a Driver with Disabilities during a Road Accident—A Numerical Approach
Next Article in Special Issue
Realization of Microfluidic Preconcentrator for N-Pentane Traces Impurities from the Gaseous Media
Previous Article in Journal
Supportless Lattice Structure for Additive Manufacturing of Functional Products and the Evaluation of Its Mechanical Property at Variable Strain Rates
Previous Article in Special Issue
Novel Nd-N/TiO2 Nanoparticles for Photocatalytic and Antioxidant Applications Using Hydrothermal Approach
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Structural, Magnetic, and Electrical Properties of CoFe2O4 Nanostructures Synthesized Using Microwave-Assisted Hydrothermal Method

1
Department of Physics, College of Science, King Faisal University, P.O. Box 400, Al-Ahsa 31982, Saudi Arabia
2
Department of Physics, University of Petroleum & Energy Studies, Dehradun 248007, Uttarakhand, India
3
Physics Department, Faculty of Science, Assiut University, Assiut 71516, Egypt
4
University School of Basic and Applied Sciences, Guru Gobind Singh Indraprastha University, New Delhi 110078, India
5
Department of Basic Sciences, Preparatory Year Deanship, King Faisal University, P.O. Box 400, Al-Ahsa 31982, Saudi Arabia
6
Department of Pure & Applied Physics, University of Kota, Kota 324005, Rajasthan, India
7
Basic Science Department, Pre-Professional Program-Female, College of Science and Health Profession, King Saud bin Abdul Aziz University for Health Sciences, Al-Ahsa 31982, Saudi Arabia
8
Department of Applied Physics, Aligarh Muslim University, Aligarh 202001, Uttar Pradesh, India
9
School of Materials Science and Engineering, Changwon National University, Changwon 51140, Gyeongnam, Korea
*
Author to whom correspondence should be addressed.
Materials 2022, 15(22), 7955; https://doi.org/10.3390/ma15227955
Submission received: 22 October 2022 / Revised: 2 November 2022 / Accepted: 8 November 2022 / Published: 10 November 2022

Abstract

:
Magnetic nanostructures of CoFe2O4 were synthesized via a microwave-assisted hydrothermal route. The prepared nanostructures were investigated using X-ray diffraction (XRD), field emission electron microscopy (FE-SEM), energy dispersive X-ray (EDX) spectroscopy, high-resolution transmission electron microscopy (HR-TEM), selective area electron diffraction (SAED) pattern, DC magnetization, and dielectric spectroscopy measurements. The crystal structure studied using HR-TEM, SAED, and XRD patterns revealed that the synthesized nanostructures had a single-phase nature and ruled out the possibility of any secondary phase. The lattice parameters and unit cell volume determined from the XRD data were found to be 8.4821 Å and 583.88 Å3. The average crystallite size (~7.0 nm) was determined using Scherrer’s equation. The FE-SEM and TEM micrographs revealed that the prepared nanostructures had a spherical shape morphology. The EDX results showed that the major elements present in the samples were Co, Fe, and O. The magnetization (M) versus temperature (T) measurements specified that the CoFe2O4 nanostructures showed ferromagnetic ordering at room temperature. The blocking temperature (TB) determined using the M-T curve was found to be 315 K. The magnetic hysteresis (M-H) loop of the CoFe2O4 nanostructures recorded at different temperatures showed the ferromagnetic behavior of the CoFe2O4 nanostructures at temperatures of 200 K and 300 K, and a superparamagnetic behavior at 350 K. The dielectric spectroscopy studies revealed a dielectric constant (ε′) and loss tangent (tanδ) decrease with the increase in the frequency, as well as demonstrating a normal dispersion behavior, which is due to the Maxwell–Wagner type of interfacial polarization. The values of ε′ and tanδ were observed to increase with the increase in the temperature.

1. Introduction

Magnetic nanostructures have received widespread attention from researchers, due to their underlying chemical and physical properties, as well as for potential technological applications [1,2,3,4,5,6,7]. These magnetic nanostructures display remarkable electrical and magnetic properties compared to their bulk counterparts. It has been observed that magnetic nanostructures have numerous exceptional features in the nanometer range, due to strong modifications occurring at in surface/interfaces as compared to the bulk material. Magnetic materials display various unique properties adaptable to modulations, such as saturation magnetization, superparamagnetism, coercivity, spin-glass behavior, etc. [8,9,10,11,12]. Moreover, the design and growth of magnetic nanostructures have become a central point for researchers in applied research, because of their unusual and superior structural properties. In particular, spinel ferrite with an AB2O4 type crystal structure has shown remarkable magnetic and dielectric properties in its nanocrystalline shape compared to bulk particles and has demonstrated technological applications in various fields, such as for biomedical fields, chemical stability, storage media, high electrical resistivity, magnetic nanofluids, high-pressure sensors through Cr3+ doping, magnetic resonance imaging, mechanical hardness, multilayer chip indicators, super-hard materials, high-temperature ceramics, etc. [13,14,15,16,17,18,19]. Furthermore, it has been observed that, owing to their excellent dielectric properties, spinel ferrites possess numerous applications in radio, as well as microwave, frequency devices. Notably, the dielectric and magnetic properties of these ferrites show sensitivity towards the method of preparation and sintering conditions. Many groups have explored ferrites in the nanodomain widely because they demonstrate enhanced properties at low grain sizes [20,21,22,23]. Various techniques, such as sol-gel, hydrothermal, solvothermal, and microwave hydrothermal, etc., have developed for spinel ferrite nanostructures [24,25,26]. CoFe2O4 is a spinel ferrites that is an eminent hard magnetic material with ferromagnetic behavior, with a high Curie temperature (~793 K), strong magnetocrystalline anisotropy along with a moderate magnetization (Ms), and high coercivity (Hc). These properties of CoFe2O4 indicate its suitability for magnetic recording applications, in high-density digital recording disks, etc. The ferromagnetic ordering in CoFe2O4 results from the super-exchange interaction between the cations located in octahedral/tetrahedral sites and the oxygen anion. In this study, CoFe2O4 nanostructures were synthesized using a microwave-assisted hydrothermal procedure. The prepared nanostructures were studied using X-ray diffraction, dielectric spectroscopy, and the dc magnetization method.

2. Experimental

The microwave-assisted hydrothermal technique was employed in the synthesis of CoFe2O4 nanostructures. All chemicals were of analytical grade, purchased from Sigma–Aldrich, and used without any further treatment. In a typical synthesis, a solution of 2:1 stoichiometric molar ratio of Iron (III) nitrate nonahydrate and Cobalt(II) nitrate hexahydrate was dissolved in 50 mL de-ionized water under constant magnetic starring. Thereafter, the solution was made alkaline by adding NH4OH dropwise to reach a pH level of 9. After stirring for 1 h at room temperature, the solution was finally transferred into a Teflon vessel and was kept at 200 °C in a microwave hydrothermal for 5 min. The solution was allowed to cool at room temperature after microwave processing. The precipitate obtained via centrifugation was washed using deionized water and absolute ethanol five times and separated by centrifugation at 4000 rpm. Finally, the precipitate was dried in a hot oven at 80 °C for 2 h. The phase of the as-obtained product was characterized by X-ray diffraction (XRD) using a Phillips X’pert (MPD-3040) diffractometer (λCu = 1.5406 Å) operated at a voltage of 40 kV and current of 30 mA. Field emission scanning electron microscopy (FESEM) images were obtained using a MIRA II LMH microscope. The contribution of elements in CoFe2O4 was determined by energy-dispersive X-ray spectroscopy (EDX, Inca Oxford, attached to the FESEM). The magnetic properties were studied using quantum designed PPMS. The dielectric spectroscopy studies were carried out using an Alpha-A High-Performance Frequency Analyzer. The dielectric measurements were performed at different frequencies, ranging from 1.0 Hz to 10 MHz. Before the dielectric measurements, a circular pallet of material was prepared with a diameter and thickness of ~1.0 cm and 1.5 mm, respectively. The electrode was prepared using silver paint, applied on both parallel sides of the pallet.

3. Results and Discussion

The crystalline structure and phase of the CoFe2O4 nanostructures were characterized using room temperature XRD measurements, as shown in Figure 1. The Fullproof program unitized for the Rietveld refinement process clearly inferred that the CoFe2O4 nanostructures had a single-phase nature with phase face-centered cubic (FCC) geometry and excluded the existence of any secondary phase. The theoretical and experimental data points are symbolized by red-colored and black-colored circles, respectively. Bragg’s positions corresponding to the FCC structure are highlighted using vertical lines of link color. The difference between experimental and theoretical data is represented by the blue lines. The value of χ2, which describes the quality and reliability of refinement, was 1.2. It is worth mentioning here that all the XRD peaks showed broadening, which was attributed to the nanocrystalline nature of the CoFe2O4 nanostructures. The diffraction peaks observed at 2θ = 29.92°, 35.34°, 42.9°, 57.43°, and 62.44°, and corresponding to (220), (311), (400), (333), and (440) planes were assigned to the spinel structure of CoFe2O4 nanostructures with the space group Fd3m. All the diffraction peaks indexed in the XRD pattern were analogous to the JCPDS card number 22–1086 [27]. The average particle size, D, of CeF2O4 nanostructures was determined using the highest intense peak (311), using Scherrer’s equation, D = 0.9 λ β   C o s θ [28], where β is the broadening of the diffraction peak at angle θ. The β was measured using the equation β = ( β 0 2 B 2 ) 1 2 , where β 0 highlights the full width at half maximum (FWHM) of the diffraction peaks and B refers to the instrumental broadening. The λ is the wavelength (1.5406 Å) of the X-ray used to record the pattern. The diffraction peaks were fit by the mean of the Voigt function. The particle size evaluated using the high-intensity low angle (311) and high angle (440) peaks were found to be ~7.0 nm. The lattice parameter (a) was also calculated using the formula a = d h k l ( h 2 + k 2 + l 2 ) , here (h, k, l), represents the miller indices whereas dhkl denotes the interplaner spacing determined using the XRD pattern. The lattice parameter estimated using the (311) peak was found to be 8.3581 Å. Furthermore, the X-ray density (theoretical) was also calculated using the formula in [29], dhkl = 8M/Na3, where M stands for the molecular weight of CoFe2O4 and N denotes the Avogadro number, whereas a highlights the lattice constant and where 8 represents the number of atoms per unit cell. The X-ray density was found to be ~5.649 g/cm3.
The surface morphology of the CoFe2O4 nanostructures recorded using field emission electron microscopy (FE-SEM) is shown in Figure 2a. The FE-SEM image shows that CoFe2O4 exhibited a spherical shape morphology and revealed its nanocrystalline nature. The particle size calculated from the FE-SEM micrograph (see Figure 2b) using Image-J software was found to be 11.0 nm. The EDS spectrum of the CoFe2O4 nanostructures is displayed in Figure 2c. The ratio of Co:Fe (Figure 3c) observed from the EDX spectrum was ~1:2, indicating that the stoichiometric proportion was maintained.
Additionally, the morphology of CoFe2O4 nanostructures was further determined using transmission electron microscopy (TEM), as shown in Figure 2d. The TEM micrograph reveals that CoFe2O4 had a nanocrystalline behavior and is in good agreement with the FE-SEM and XRD results. In addition, the crystal structure of the CoFe2O4 nanostructures was again confirmed using high-resolution transmission electron microscopy and the selective area electron diffraction (SAED) pattern. The rings observed in the SAED pattern (see Figure 2f) were successfully recognized and assigned to (220), (311), (400), and (440) orientations. The interplanar distance determined using HR-TEM (see Figure 2e) was observed to be 0.26 nm, which matches with the (311) plane of the FCC crystal structure. Hence, it is possible to say that the HR-TEM, SAED, and XRD results signify that the CoFe2O4 nanostructures were successfully prepared, without any impurity phase.
Figure 3 demonstrates the magnetization versus temperature (M-T) measurement of the CoFe2O4 nanostructures. The M-T measurements, performed in zero-field-cooled (ZFC) and field-cooled (FC) measurements mode, followed a procedure in which the sample was cooled from 300 K to 50 K in the absence of (ZFC); thereafter, a static magnetic field of 500 Oe was applied and the magnetization was recorded during the warming-up cycle. Then, the sample was cooled from 300 K to 50 K in the presence of the magnetic field of 500 Oe (FC) and the magnetization was measured in the warming-up cycle. The ZFC–FC measurements indicated that the CoFe2O4 nanostructures showed ferromagnetic ordering at room temperature, with a blocking temperature (TB) of 315 K, which is a transition from a superparamagnetic state to a blocked state. Here, it is worth mentioning that a change in FC and ZFC magnetization below 315 K resulted from the energy barriers of the magnetic anisotropy [30]. The TB of magnetic materials depends on the interparticle magnetic interactions, as well as particle size. With the help of TB and the volume of the single particle, the magnetic anisotropy constant K was calculated using the formula ( K = 25 K B T B V ) and observed to be 3.2 × 105 J/m3, where K B is Boltzmann’s constant.
Figure 4 represents the magnetic hysteresis (M-H) loop of CoFe2O4 nanostructures measured at different temperatures. It can be observed that the CoFe2O4 nanostructures demonstrated ferromagnetic behavior at temperatures 200 K and 300 K, whereas the reversible M-H curve at 350 K reflects a superparamagnetic behavior. From Figure 4, it is evident that the area under the hysteresis loop increased with a decrease in the temperature. The values coercive field (HC) and remanence magnetization (MR) calculated from the hysteresis loop were 755 Oe and 16 emu/g at 200 K, and 91.0 Oe and 3.7 emu/g at 300 K, respectively. It can be observed from Figure 4 that the magnetization was unsaturated until applying 5 T. Therefore, the MS was calculated by extrapolating the M versus H/T curves. The saturation magnetizations (MS) calculated using M-H loops were 50.0 emu/g, 48.0 emu/g, and 46.0 emu/g at 200 K, 300 K, and 350 K, respectively. The values of the various magnetic parameters (see Table 1) were found to decrease with an increase in temperature. This can be attributed to the decrease in the exchange interactions between the spin moments, because of the thermal activation energy.
Figure 5 depicts the dielectric constant (ε′) versus the frequency curve, showing the real part of the dielectric constant of CoFe2O4 nanostructures measured at different temperatures in the frequency range of 1.0 Hz to 10 MHz. The value of the dielectric constant was determined using the formula ε = C p × d ε 0 × A , where d is the thickness of the pellet, C p is the capacitance of the parallel pellet, A is the cross-sectional area of the painted surface, and ε 0 is the space permittivity of free space. The value of ε′, as shown in Table 2, was found to increase with the increase in the temperature. Additionally, the dielectric constant was found to decrease, as observed in Figure 5, with an increase in frequency, which is the usual behavior reported for most polar dielectric materials [31]. However, it was noticed that the decreasing behavior became slower at the higher frequencies and showed an almost frequency-independent behavior. This type of frequency-dependent nature of ε′ can be interpreted using the Maxwell–Wagner two-layer model, which is consistent with Koop’s theory of dielectrics [15]. Koop’s model explains that dielectric materials are made-up of conducting grains, as well as insulating grain boundaries. It is reported that grain boundaries result in ferrites because of the oxidation of superficial reduction of crystallites as a result of the sintering process [32,33,34,35]. When dielectric measurements are performed in the alternating field, the grain boundaries dominate at lower frequencies, whereas high conductive grains are effective at high frequencies. Therefore, the voltage applied to the specimen drops predominantly on both sides of the grain boundaries and causes space charge polarization, since the hopping of electrons inside the material accumulates at the grain boundaries because of high grain boundary resistance. The large value of the ε′ in CoFe2O4 nanostructures is ascribed to the greater effect grain boundaries have over grains than at lower frequencies, which indicates the major role of space charge polarization. However, the ε′ starts to decrease as the frequency increases further, because of the weak space charge polarization. At high frequencies, electrons lag behind, while following the changes of the applied field exchange, and thus ε′ decreases and become steady beyond a certain frequency limit. Figure 6 highlights dielectric loss (tanδ) versus frequency of CoFe2O4 nanostructures. The dielectric loss was measured in the frequency range of 1.0 Hz to 10 MHz at different temperatures. The dielectric loss tangent ((tanδ) can be determined using the formula t a n δ = ε ε , where ε is the complex dielectric constant. The dielectric loss tangent (tanδ) signifies the loss of energy from the applied field into the material and that is dissipated in the form of heat energy. It was found that the dielectric loss decreased with an increase in frequency of the applied field, indicating a normal dispersion behavior. It can be seen from Figure 6 that tanδ has a low loss value at higher frequencies, which shows its suitability for applications in high frequency devices. The high value of tanδ at low frequency may be because of its high resistivity (owing to grain boundary). Since the electrons’ hopping among Fe2+ ⇔ Fe3+, as well as hole transfer involving Co2+ ⇔ Co3+, require more energy, this causes the high value of tanδ. Moreover, in the high frequency region, the hopping of electrons requires little energy, due to the low resistivity (because of grains), and as a result, the loss is small. Furthermore, the value of tanδ is also dependent on other factors, such as the sintering temperature of the material, composition, structural homogeneity, and the Fe2+ and Fe3+ content in samples. Additionally, it can be noticed that the values ε′ and tanδ increase with temperature and display a semiconducting behavior (See Table 2). This may be due to the fact that, at low temperatures, the charge carriers do not have sufficient energy and because of that cannot orient themselves along the course of the applied field variation and, hence, contribute weakly to the polarization. An increase in temperature causes the charge carries to obtain sufficient thermal energy and they start to follow the change in the externally applied field, and as a result of this, the dielectric constant increases.
Furthermore, the ac-conductivity observed in the dielectric materials can be measured in relation with the frequency using the following equation: σac = є’ єoω tanδ, where the symbols have their usual meaning [36,37]. The ac conductivity was observed to increase with an increase in the temperature (see Table 2). The frequency-dependent ac-conductivity curves of CoFe2O4 are displayed in Figure 7, in the frequency range of 1.0–10.0 MHz. The curves demonstrate that the ac-conductivity substantially follows the frequency, and showing a good correlation between the two. The increase of ac-conductivity with frequency may be associated with the possible reduction in the resistance present at the grain boundaries, which was developed due to the charge accumulation at the opposite sides of the grain boundaries. The short-grain boundaries may have reduced the resistance and enhanced the ac-conductivity with the frequency.

4. Conclusions

We successfully prepared CoFe2O4 nanostructures using a microwave-supported hydrothermal route. The crystal structure studied using HR-TEM, XRD, and SAED spectra confirmed the single-phase nature, with an FCC structure. Crystallographic parameters, such as the lattice parameters and unit cell volume, calculated using Rietveld refinement of XRD data were 8.4821 Å and 583.88 Å3, respectively. The average crystallite size measured using the FE-SEM and XRD data was 11.0 nm and 7.0 nm, respectively. The spherical type morphology of CoFe2O4 nanostructures was observed from the TEM and FE-SEM micrographs. The ZFC and FC studies of CoFe2O4 nanostructures indicated ferromagnetic ordering at room temperature, along with a TB of ~315 K. The M-H measurements showed that the CoFe2O4 nanostructures demonstrated a superparamagnetic behavior above room temperature. It was observed that with an increase in frequency, the dielectric constant and loss tangent were found to decrease. However, the dielectric constant and loss tangent were observed to increase with an increase in temperature.

Author Contributions

Data curation, S.K., F.A. and F.S.; Formal analysis, S.K., F.A., R.K., N.A., S.D. (Saurabh Dalela), S.D. (Sourabh Dwivedi) and K.K.; Funding acquisition, S.K.; Investigation, N.M.S., R.K., S.D. (Saurabh Dalela), F.S., S.D. (Sourabh Dwivedi) and K.K.; Methodology, N.M.S. and N.A.; Project administration, A.A.; Resources, A.A.; Visualization, S.K.; Writing—original draft, S.K. and K.K.; Writing—review and editing, F.A., N.M.S., R.K., A.A., N.A., S.D. (Sourabh Dwivedi), F.S., S.D. (Sourabh Dwivedi) and K.K. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by Deanship of Scientific Research, Vice Presidency for Graduate Studies and Scientific Research, King Faisal University, Saudi Arabia [Project No. GRANT852].

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Available on request.

Acknowledgments

This work was supported by the Deanship of Scientific Research, Vice Presidency for Graduate Studies and Scientific Research, King Faisal University, Saudi Arabia [Project No. GRANT852].

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Mohamed Racik, K.; Anand, S.; Muniyappan, S.; Nandhini, S.; Rameshkumar, S.; Mani, D.; Karuppasamy, P.; Pandian, M.S.; Ramasamy, P. Preparation of CoFe2O4/SiO2 nanocomposite as potential electrode materials for supercapacitors. Inorg. Chem. Commun. 2022, 146, 110036. [Google Scholar] [CrossRef]
  2. Mathew, T.; Shylesh, S.; Reddy, S.N.; Sebastian, C.P.; Date, S.K.; Rao, B.S.; Kulkarni, S.D. Redistribution of cations amongst different lattice sites in Cu1-xCoxFe2O4 ferrospinels during alkylation: Magnetic study. Catal. Lett. 2004, 93, 155–163. [Google Scholar] [CrossRef]
  3. Lee, S.J.; Song, S.H.; Lo, C.C.; Aldini, S.T.; Jiles, D.C. Magneto-optic properties of CoFe2-xGaxO4 J. Appl. Phys. 2007, 101, 9–11. [Google Scholar] [CrossRef] [Green Version]
  4. Nakagomi, F.; Da Silva, S.W.; Garg, V.K.; Oliveira, A.C.; Morais, P.C.; Franco Júnior, A.; Lima, E.C.D. The influence of cobalt population on the structural properties of CoxFe3-xO4 J. Appl. Phys. 2007, 101, 9–11. [Google Scholar] [CrossRef]
  5. Stewart, S.J.; Figueroa, S.J.A.; Ramallo López, J.M.; Marchetti, S.G.; Bengoa, J.F.; Prado, R.J.; Requejo, F.G. Cationic exchange in nanosized ZnFe2O4 spinel revealed by experimental and simulated near-edge absorption structure. Phys. Rev. B 2007, 75, 073408. [Google Scholar] [CrossRef] [Green Version]
  6. Kumar, S.; Srivastava, G.; Almutairi, G.; Ahmed, F.; Shaalan, N.M.; Dalela, S.; Kumar, R.; Kumar, A.P.; Alvi, P.A.; Chae, K.H.; et al. Structure and electrochemical properties of La-doped BiFeO3 nanoparticles. J. Electron. Spectros. Relat. Phenom. 2021, 253, 147138. [Google Scholar] [CrossRef]
  7. Hashim, M.; Alimuddin Kumar, S.; Shirsath, S.E.; Mohammed, E.M.; Chung, H.; Kumar, R. Studies on the activation energy from the ac conductivity measurements of rubber ferrite composites containing manganese zinc ferrite. Phys. B Condens. Matter. 2012, 407, 4097–4103. [Google Scholar] [CrossRef]
  8. Liu, K.; Baker, S.M.; Tuominen, M.; Russell, T.P.; Schuller, I.K. Tailoring exchange bias with magnetic nanostructures. Phys. Rev. B 2001, 63, 604031–604034. [Google Scholar] [CrossRef] [Green Version]
  9. Shirsath, S.E.; Liu, X.; Yasukawa, Y.; Li, S.; Morisako, A. Switching of magnetic easy-axis using crystal orientation for large perpendicular coercivity in CoFe2O4 thin film. Sci. Rep. 2016, 6, 30074. [Google Scholar] [CrossRef] [Green Version]
  10. Park, J.; Joo, J.; Soon, G.K.; Jang, Y.; Hyeon, T. Synthesis of monodisperse spherical nanocrystal. Angew. Chem. Int. Ed. 2007, 46, 4630–4660. [Google Scholar] [CrossRef] [PubMed]
  11. Anjum, G.; Kumar, R.; Mollah, S.; Shukla, D.K.; Kumar, S.; Lee, C.G. Structural, dielectric, and magnetic properties of La0.8Bi0.2Fe1−xMnxO3 (0.0 ≤ x ≤ 0.4) multiferroics. J. Appl. Phys. 2010, 107, 103916. [Google Scholar] [CrossRef] [Green Version]
  12. Kumari, A.; Kumari, K.; Aljawfi, R.N.; Alvi, P.A.; Dalela, S.; Ahmad, M.M.; Chawla, A.K.; Kumar, R.; Vij, A.; Kumar, S. Role of La substitution on structural, optical, and multiferroic properties of BiFeO3 nanoparticles. Appl. Nanosci. 2021, 1–20. [Google Scholar] [CrossRef]
  13. Wang, Z.; Downs, T.; Pischedda, V.; Shetty, R.; Saxena, K.; Zha, S.; Zhao, S.; Schiferl, D.; Waskowska, A. High-pressure X-ray diffraction and Raman spectroscopic studies of the tetragonal spinel CoFe2O4. Phys. Rev. B 2003, 68, 2–7. [Google Scholar]
  14. Hashim, M.; Alimuddin Kumar, S.; Shirsath, S.E.; Kotnala, R.K.; Chung, H.; Kumar, R. Structural properties and magnetic interactions in Ni0.5Mg0.5Fe2-xCrxO4 (0 ≤ x ≤ 1) ferrite nanoparticles. Powder Technol. 2012, 229, 37–44. [Google Scholar] [CrossRef]
  15. Kumar, S.; Alimuddin Kumar, R.; Thakur, P.; Chae, K.H.; Angadi, B.; Choi, W.K. Electrical transport, magnetic, and electronic structure studies of Mg0.95Mn0.05Fe2−2xTi2xO4 ± δ (0 ≤ x ≤ 0.5) ferrites. J. Phys. Condens. Matter 2007, 19, 476210. [Google Scholar] [CrossRef]
  16. Hashim, M.; Shirsath, S.E.; Meena, S.S.; Mane, M.L.; Kumar, S.; Bhatt, P.; Kumar, R.; Prasad, N.K.; Alla, S.K.; Shah, J.; et al. Manganese ferrite prepared using reverse micelle process: Structural and magnetic properties characterization. J. Alloy. Compd. 2015, 642, 70–77. [Google Scholar] [CrossRef]
  17. Zerr, A.; Miehe, G.; Serghiou, G.; Schwarz, M.; Kroke, E.; Riedel, R.; Fueß, H.; Kroll, P.; Boehler, R. Synthesis of cubic silicon nitride. Nature 1999, 400, 340–342. [Google Scholar] [CrossRef]
  18. Sharma, S.K.; Kumar, R.; Kumar, S.; Siva Kumar, V.V.; Knobel, M.; Reddy, V.R.; Banerjee, A.; Singh, M. Magnetic study of Mg0.95Mn0.05Fe2O4 ferrite nanoparticles. Solid State Commun. 2007, 141, 203–208. [Google Scholar] [CrossRef]
  19. Kumar, S.; Farea, A.M.M.; Batoo, K.M.; Lee, C.G.; Koo, B.H.; Yousef, A.; Alimuddi. Mössbauer studies of Co0.5CdxFe2.5−xO4 (0.0 ⩽ x ⩽ 0.5) ferrite. Phys. B Condens. Matter 2008, 403, 3604–3607. [Google Scholar] [CrossRef]
  20. Bayoumi, W. Structural and electrical properties of zinc-substituted cobalt ferrite. J. Mater. Sci. 2007, 42, 8254–8261. [Google Scholar] [CrossRef]
  21. Patil, A.N.; Patil, M.G.; Patankar, K.K.; Mathe, V.L.; Mahajan, R.P.; Patil, S.A. Dielectric behaviour and a.c. conductivity in CuxFe3-xO4 ferrite. Bull. Mater. Sci. 2000, 23, 447–452. [Google Scholar] [CrossRef]
  22. Rane, K.S.; Verenkar VM, S.; Sawant, P.Y. Dielectric behaviour of MgFe2O4 prepared from chemically beneficiated iron ore rejects. Bull. Mater. Sci. 2001, 24, 323–330. [Google Scholar] [CrossRef]
  23. Ušáková, M.; Lukáč, J.; Dosoudil, R.; Jančárik, V.; Grusková, A.; Ušák, E.; Sláma, J.; Šubrt, J. Influence of Cu2+ ions on structural and magnetic properties of NiZn ferrites. J. Mater. Sci. Mater. Electron. 2007, 18, 1183–1189. [Google Scholar] [CrossRef]
  24. Pillai, V.; Shah, D.O. Synthesis of high-coercivity cobalt ferrite particles using water-in-oil microemulsions. J. Magn. Magn. Mater. 1996, 163, 243–248. [Google Scholar] [CrossRef]
  25. Ahn, Y.; Choi, E.J.; Kim, S.; Ok, H.N. Magnetization and Mössbauer study of cobalt ferrite particles from nanophase cobalt iron carbonate. Mater. Lett. 2001, 50, 47–52. [Google Scholar] [CrossRef]
  26. Sharma, S.K.; Kumar, R.; Kumar, S.; Knobel, M.; Meneses, C.T.; Siva Kumar, V.V.; Reddy, V.R.; Singh, M.; Lee, C.G. Role of interparticle interactions on the magnetic behavior of Mg0.95Mn0.05Fe2O4 ferrite nanoparticles. J. Phys. Condens. Matter 2008, 20, 235214. [Google Scholar] [CrossRef] [PubMed]
  27. Sedlacik, M.; Pavlinek, V.; Peer, P.; Filip, P. Tailoring the magnetic properties and magnetorheological behavior of spinel nanocrystalline cobalt ferrite by varying annealing temperature. Dalt. Trans. 2014, 43, 6919–6924. [Google Scholar] [CrossRef] [Green Version]
  28. Kumari, K.; Aljawfi, R.N.; Chawla, A.K.; Kumar, R.; Alvi, P.A.; Alshoaibi, A.; Vij, A.; Ahmed, F.; Abu-samak, M.; Kumar, S. Engineering the optical properties of Cu doped CeO2 NCs for application in white LED. Ceram. Int. 2020, 46, 7482–7488. [Google Scholar] [CrossRef]
  29. Sahu, J.; Kumar, S.; Vats, V.S.; Alvi, P.A.; Dalela, B.; Kumar, S.; Phase, D.M.; Gupta, M.; Dalela, S. Exploring the Defects and Vacancies with Photoluminescence and XANES Studies of Gd3+-Substituted ZnO Nanoparticles. Part. Part. Syst. Charact. 2022, 39, 2200116. [Google Scholar] [CrossRef]
  30. Mahhouti, Z.; El Moussaoui, H.; Mahfoud, T.; Hamedoun, M.; El Marssi, M.; Lahmar, A.; El Kenz, A.; Benyoussef, A. Chemical synthesis and magnetic properties of monodisperse cobalt ferrite nanoparticles. J. Mater. Sci. Mater. Electron. 2019, 30, 14913–14922. [Google Scholar] [CrossRef] [Green Version]
  31. Cernea, M.; Galizia, P.; Ciuchi, I.; Aldica, G.; Mihalache, V.; Diamandescu, L.; Galassi, C. CoFe2O4 magnetic ceramic derived from gel and densified by spark plasma sintering. J. Alloys Compd. 2016, 656, 854–862. [Google Scholar] [CrossRef]
  32. Koops, C.G. On the Dispersion of Resistivity and Dielectric Constant of Some Semiconductors at Audiofrequencies. Phys. Rev. 1951, 83, 121–124. [Google Scholar] [CrossRef]
  33. Asandulesa, M.; Kostromin, S.; Podshivalov, A.; Tameev, A.; Bronnikov, S. Relaxation processes in a polymer composite for bulk heterojunction: A dielectric spectroscopy study. Polymer 2020, 203, 122785. [Google Scholar] [CrossRef]
  34. Reddy, P.V.; Rao, T.S. Dielectric behaviour of mixed Li-Ni ferrites at low frequencies. J. Less Common Met. 1982, 86, 255–261. [Google Scholar] [CrossRef]
  35. Asandulesa, M.; Chibac-Scutaru, A.L.; Culica, M.E.; Melinte, V.; Coseri, S. Cellulose-based films with enhanced load of nitrogen containing heterocycles: The impact on the surface morphology and proton conductivity. Appl. Surf. Sci. 2023, 607, 155077. [Google Scholar] [CrossRef]
  36. Kumari, A.; Kumari, K.; Ahmed, F.; Alshoaibi, A.; Alvi, P.A.; Dalela, S.; Ahmad, M.M.; Aljawfi, R.N.; Dua, P.; Vij, A.; et al. Influence of Sm doping on structural, ferroelectric, electrical, optical and magnetic properties of BaTiO3. Vacuum 2021, 184, 109872. [Google Scholar] [CrossRef]
  37. Asandulesa, M.; Kostromin, S.; Tameev, A.; Aleksandrov, A.; Bronnikov, S. Molecular Dynamics and Conductivity of a PTB7:PC71BM Photovoltaic Polymer Blend: A Dielectric Spectroscopy Study. ACS Appl. Polym. Mater. 2021, 3, 4869–4878. [Google Scholar] [CrossRef]
Figure 1. X-ray diffraction pattern of CeFe2O4 nanostructures measured at room temperature.
Figure 1. X-ray diffraction pattern of CeFe2O4 nanostructures measured at room temperature.
Materials 15 07955 g001
Figure 2. (a) Field emission scanning electron microscopy (FE-SEM) micrograph of CeFe2O4 nanostructures, (b) particle size distribution histogram of CeFe2O4 nanostructures, (c) energy-dispersive X-ray spectroscopy (EDS) spectrum of CoFe2O4 nanostructures and the stoichiometry (%) of constituent elements present in CeFe2O4 nanostructures. (d) Transmission electron microscopy (TEM) micrograph of CeFe2O4 nanostructures, (e) high-resolution transmission electron microscopy (HR-TEM) micrograph of CeFe2O4 nanostructures, (f) selective area electron diffraction (SAED) pattern of CeFe2O4 nanostructures.
Figure 2. (a) Field emission scanning electron microscopy (FE-SEM) micrograph of CeFe2O4 nanostructures, (b) particle size distribution histogram of CeFe2O4 nanostructures, (c) energy-dispersive X-ray spectroscopy (EDS) spectrum of CoFe2O4 nanostructures and the stoichiometry (%) of constituent elements present in CeFe2O4 nanostructures. (d) Transmission electron microscopy (TEM) micrograph of CeFe2O4 nanostructures, (e) high-resolution transmission electron microscopy (HR-TEM) micrograph of CeFe2O4 nanostructures, (f) selective area electron diffraction (SAED) pattern of CeFe2O4 nanostructures.
Materials 15 07955 g002
Figure 3. Field-cooled (FC) and zero-field-cooled (ZFC) magnetization versus temperature curves of CeFe2O4 nanostructures measured in a magnetic field of 500 Oe.
Figure 3. Field-cooled (FC) and zero-field-cooled (ZFC) magnetization versus temperature curves of CeFe2O4 nanostructures measured in a magnetic field of 500 Oe.
Materials 15 07955 g003
Figure 4. Hysteresis loops of CeFe2O4 nanostructures at different temperatures.
Figure 4. Hysteresis loops of CeFe2O4 nanostructures at different temperatures.
Materials 15 07955 g004
Figure 5. Dielectric constant versus frequency curve of CeFe2O4 nanostructures at different temperatures.
Figure 5. Dielectric constant versus frequency curve of CeFe2O4 nanostructures at different temperatures.
Materials 15 07955 g005
Figure 6. Loss tangent (tanδ) versus frequency curve of CeFe2O4 nanostructures at different temperatures.
Figure 6. Loss tangent (tanδ) versus frequency curve of CeFe2O4 nanostructures at different temperatures.
Materials 15 07955 g006
Figure 7. σac versus frequency curve of CeFe2O4 nanostructures at different temperatures. Inset shows log (σac) versus log (frequency) curve of CeFe2O4 nanostructures at different temperatures.
Figure 7. σac versus frequency curve of CeFe2O4 nanostructures at different temperatures. Inset shows log (σac) versus log (frequency) curve of CeFe2O4 nanostructures at different temperatures.
Materials 15 07955 g007
Table 1. Saturation magnetization (Ms), and remanence magnetization (MR), coercive field (HC) of CeFe2O4 nanostructures calculated from M-H curve at different temperatures.
Table 1. Saturation magnetization (Ms), and remanence magnetization (MR), coercive field (HC) of CeFe2O4 nanostructures calculated from M-H curve at different temperatures.
200 K300 K350 K
MS (emu/g)504846
MR (emu/g)163.70
HC (Oe)755910
Table 2. Dielectric constant (ε′), loss tangent (tanδ), and ac conductivity (σac) CoFe2O4 nanostructures recorded at 1.0 MHz.
Table 2. Dielectric constant (ε′), loss tangent (tanδ), and ac conductivity (σac) CoFe2O4 nanostructures recorded at 1.0 MHz.
CoFe2O4133 K233 K273 K323 K373 K
Dielectric constant (ε′)11.411.812.414.320.8
Loss tangent (tanδ)4.6 × 10−41.4 × 10−35.0 × 10−20.230.82
ac conductivity (σac)1.2 × 10−81.1 × 10−74.8 × 10−72.4 × 10−61.2 × 10−5
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Kumar, S.; Ahmed, F.; Shaalan, N.M.; Kumar, R.; Alshoaibi, A.; Arshi, N.; Dalela, S.; Sayeed, F.; Dwivedi, S.; Kumari, K. Structural, Magnetic, and Electrical Properties of CoFe2O4 Nanostructures Synthesized Using Microwave-Assisted Hydrothermal Method. Materials 2022, 15, 7955. https://doi.org/10.3390/ma15227955

AMA Style

Kumar S, Ahmed F, Shaalan NM, Kumar R, Alshoaibi A, Arshi N, Dalela S, Sayeed F, Dwivedi S, Kumari K. Structural, Magnetic, and Electrical Properties of CoFe2O4 Nanostructures Synthesized Using Microwave-Assisted Hydrothermal Method. Materials. 2022; 15(22):7955. https://doi.org/10.3390/ma15227955

Chicago/Turabian Style

Kumar, Shalendra, Faheem Ahmed, Nagih M. Shaalan, Rajesh Kumar, Adil Alshoaibi, Nishat Arshi, Saurabh Dalela, Fatima Sayeed, Sourabh Dwivedi, and Kavita Kumari. 2022. "Structural, Magnetic, and Electrical Properties of CoFe2O4 Nanostructures Synthesized Using Microwave-Assisted Hydrothermal Method" Materials 15, no. 22: 7955. https://doi.org/10.3390/ma15227955

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop