Abstract
1. Introduction
In 2000, Subramanian et al.[
Varistors are voltage-dependent resistors that demonstrate strong nonlinear current versus voltage (I–V) characteristics. The electrical properties of varistors are chiefly influenced by grain-boundary interface states. The principal function of a varistor is to sense and control transient voltage surges. When a varistor is subjected to a high applied voltage, its impedance changes from a near open circuit to a highly conducting state, which results in the clamping of the transient voltage to a safe level and thus electronic components of high-cost electronic devices may be protected. Between 2016 and 2021, a limited number of research reports were published on J–E characteristics of CaCu3Ti4O12 cubic perovskites substituted with different metallic cation/cations. For example, the nonlinear electrical properties with high-performance dielectric behavior of CaCu2.95Cr0.05Ti4.1O12 have been studied by Prompa et al.[
Based on the following facts, the work presented in this communication is important as well as different from the existing literature. The electrical properties, J–E characteristics and dc resistivity of CaCu3–xTi4–xFe2xO12 with x = 0.0, 0.1, 0.3, 0.5, and 0.7 have been studied over a wide temperature range of T = 313 to 773 K as a function of Fe-concentration (x). The compositional variation of various electrical parameters (e.g., maximum current density, breakdown electric field, the temperature at which switching action takes place, Schottky barrier height, non-linearity coefficient, and activation energy) are determined and correlated with structural parameters (i.e., lattice constant, cationic distribution), microstructural parameters (i.e., grain size, microstrain, dislocation density) and positron annihilation lifetime (PAL) parameters (i.e., defect-specific positron lifetime, the concentration of vacancy defect). We have thoroughly investigated various physical properties of pristine and Fe3+-substituted CaCu3Ti4O12 ceramics, CaCu3–xTi4–xFe2xO12 with x = 0.0–0.7, in recent years (2018–2021)[
2. Experimental details
A series of cubic perovskites, CaCu3–xTi4–xFe2xO12 with x = 0.0, 0.1, 0.3, 0.5 and 0.7, was prepared by the mixed oxide route. The complete details regarding the synthesis, crystallographic phase identification, and structural parameters including cationic distribution determination by employing Rietveld refinement of X-ray powder diffraction data and average grain size (D) estimation by analyzing scanning electron micrographs are given elsewhere[
3. Results and discussion
A careful structural analysis demonstrates that the x = 0.0–0.5 compositions are formed in the single phase with cubic perovskite crystal symmetry in the space group Im3. For the composition with x = 0.7, the aciculate but low intensity (~ 4.0 %) peak centered at 2θ = 25.6° is due to a trivial amount of anatase structure of well-crystallized TiO2[
Fig. 1 gives the plots of J against E registered at different temperatures ranging from T = 300–773 K for the series CaCu3–xTi4–xFe2xO12. The samples exhibit strong non-ohmic characteristics. In the low E region, the dominant conduction mechanism is thermal excitation and as a result the J–E curve is nearly ohmic. Nonlinear behavior is observed when E is beyond the particular threshold value or breakdown value (Es) (E > Es). In this regime, tunneling action via grain-boundary barrier is responsible for the electric conduction. It is seen in Fig. 1 that the lowest temperature at which switching action takes place (TsL) decreases with Fe-content (x). The compositions with x = 0.0, (0.1, 0.3, 0.5) and 0.7 show switching action for T ≥ 473 K, (T ≥ 373 K),T ≥ 313 K, respectively. Meanwhile,Es decreases with x for x = 0.0 to 0.5 compositions, while for x = 0.7 composition Es shows small enhancement (Table 1). The compositional variation of Es may be described by considering the structural and microstructural parameters. The strain values have been deduced from the simple and widely employed Williamson-Hall plot method[
Figure 1.(Color online) Plots of
Figure 2.Williamson-Hall plots for all the samples of a series CaCu3–
Another interesting observation from Fig. 1 is that maximum current density (Jmax) decreases from 327 mA/cm2 for x = 0.0 composition to 270 mA/cm2 for x = 0.1 composition to 225 mA/cm2 for x = 0.3 composition and remains constant with further Fe3+-substitution. In the design of electronic and electrical devices, current density has a very significant role. Over the last few years, there has been a movement towards having a higher current density to achieve a higher number of devices in an ever-smaller chip area. As discussed earlier, with an increase in D for x = 0.0–0.5 compositions, the contribution from poorly conducting grain boundaries decreases as compared to semiconducting grains; thus, Jmax is expected to increase with Fe- substitution, but this is not the case. This suggests that besides grain size, other microstructural parameters are also expected to affect Jmax. Zheng et al.[
To the best of our knowledge, these values of Jmax for the pure and Fe-substituted CaCu3Ti4O12 ceramics are the highest ever reported values, except for those reported for Nb5+ and Ta5+-substituted CaCu3Ti4O12 (Jmax ≈ 275 mA/cm2)[
The existence of the Schottky barrier at the grain boundaries is signified by the observed linear relationship for ln J against E1/2 traces[
Figure 3.(Color online) ln
Figure 4.(Color online) Plots of ln
The coefficient of determination (R2) of a statistical model describes how well it fits a set of observations. A measure of this goodness-of-fit typically summarizes the discrepancy between the observed values and the values expected under the model in question. The R2 value between 0.70–1.0 indicates that there is a strong correlation between the dependent and independent variables. In general, R2 value at or above 0.60 is considered to be worthwhile[
On fitting ln J0 versus reciprocal of temperature (1000/T) plots with linear relation, the R2 value for x = 0.0 composition is found to be 0.91, for x = 0.1 composition,R2 = 0.94, for x = 0.3 composition, R2 = 0.97, for x = 0.5 composition, R2 = 0.95 and for the composition with x = 0.7, R2 comes to 0.90. These values of R2 are near the ideal value of 1.0, which suggests that the applied carrier transport model is able to successfully and accurately model the experimental data.
When we think about the varistor-type device, two parameters (i.e., non-linearity coefficient (α) and Es) are considered as a figure-of-merit. A large value of α is always desirable because it allows the device to withstand the surges at Es. The α values at different temperatures were calculated for the compositions with x = 0.0–0.7 using the standard definition. The α value is found to vary from 2.09–4.51, 0.45–1.14, 0.60–1.64, 0.76–2.34, and 1.27–6.88 for x = 0.0, 0.1, 0.3, 0.5 and 0.7 compositions, respectively, in the studied range of temperature. Furthermore, the value of α is found to increase with temperature and Fe-substitution (x) (x = 0.1–0.7). This can be explained as follows.
The nonlinear coefficient (
The high-temperature synthesis process of oxide ceramics that is employed here leads to the inevitable formation and existence of pores. Thus, X-ray density (dx) is always higher than the bulk density (d). These voids decisively affect the electric, dielectric, and elastic properties of the material. Thus, it is essential to correct such parameters for a void-free state, especially for compositional dependent investigation. The dc resistivity values in the void-free state (ρdc) for the different compositions have been determined from the experimental values of dc resistivity (ρp) recorded at different temperatures and void fraction values (f = 1 – (d/dx)) with the help of the following relation [
This relation is effectively applied for the materials having f < 0.4. The different compositions of the system under study possess f values that are much less than 0.4, as shown in Table 1. The ρdc values for x = 0.0–0.7 compositions lie in the range105–108 Ω·cm at T = 300 K, advising that these are good insulating materials. Fig. 5 portrays log ρ versus temperature plots (Arrhenius plot). All of the compositions reveal usual semiconducting behavior (i.e., a decrease of resistivity with temperature). In the low-temperature regime, 300 K ≤ T ≤ 573 K, a linear variation of resistivity with temperature is observed; while for T > 573 K, a discontinuity or change of slope occurs, suggesting a change in the mechanism responsible for conduction in the studied materials. This may be correlated with the diffuse anomaly that takes place at T = 630 K[
Figure 5.(Color online) Arrhenius plots for a quadruple perovskite series, CaCu3–
4. Conclusions
The following conclusions can be drawn based on the electrical properties studies of a series of quadruple perovskites, CaCu3–xTi4–xFe2xO12 where x = 0.0–0.7. The switching action is chiefly due to the concentration of Jahn-Teller Cu2+ ion engendered distortion in the system. The variation of switching temperature and threshold field is principally governed by grain size, interface defect density, and vacancy defects but not by compressive strain. The Jmax value is controlled by a change in Cu2+ ion concentration on the A´-site and the thickness of the grain-boundary layer on Fe3+-substitution. It is possible to tailor electrical parameters by controlling the structural and microstructural parameters, which is important from an application's point of view. The system is found to be suitable for low-voltage varistor applications. The compositional dependence of dc resistivity is governed by ferric ion concentration on the square-planar site of cubic perovskite structure and the activation energy values are suggestive of conduction through electrons with deformation.
Acknowledgements
One of the authors (DJP) is thankful to the Education Department, Gujarat state for providing financial assistance under ScHeme of developing high-quality research (SHODH).
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