Fe3+-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu3Ti4O12

Kunal B. Modi; Pooja Y. Raval; Dolly J. Parekh; Shrey K. Modi; Niketa P. Joshi; Akshay R. Makadiya; Nimish H. Vasoya; Utpal S. Joshi

doi:10.1088/1674-4926/43/3/032001

J. Semicond. > 2022, Volume 43 > Issue 3 > 032001

ARTICLES

Fe³⁺-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu₃Ti₄O₁₂

Kunal B. Modi^1,, Pooja Y. Raval², Dolly J. Parekh¹, Shrey K. Modi³, Niketa P. Joshi¹, Akshay R. Makadiya¹, Nimish H. Vasoya⁴ and Utpal S. Joshi⁵

+ Author Affiliations

Corresponding author: Kunal B. Modi, kunalbmodi2003@yahoo.com

DOI: 10.1088/1674-4926/43/3/032001

Abstract: The electrical properties of cubic perovskite series, CaCu_3–xTi_4–xFe_2xO₁₂ with x = 0.0, 0.1, 0.3, 0.5, and 0.7, have been studied by employing current density as a function of electric field characteristics registered at different temperatures and thermal variations of direct current electrical resistivity measurements. All of the compositions exhibit strong non-ohmic behavior. The concentration dependence of breakdown field, the temperature at which switching action takes place, and maximum value of current density (J_max) has been explained on account of structural, microstructural, and positron lifetime parameters. The highest ever reported value of J_max = 327 mA/cm² has been observed for pristine composition. The values of the nonlinear coefficient advise the suitability of ceramics for low-voltage varistor applications. The Arrhenius plots show typical semiconducting nature. The activation energy values indicate that electric conduction proceeds through electrons with deformation in the system.

Key words: perovskites, magnetic materials, J–E characteristics, capacitor

1. Introduction

In 2000, Subramanian et al.^[1] and Ramirez et al.^[2] noticed that the dielectric permittivity (ε´) of a microcrystalline sample of perovskite derivative calcium-copper-titanate (CaCu₃Ti₄O₁₂) abruptly jumps by a factor of 100 when heated above T = 90 K (at 1 kHz frequency). This material at T = 100 K exhibits a huge value of ε´ of the order of 10⁴ and ε´ becomes weakly dependent on temperature for T = 100–320 K. These unusual and fascinating properties make them suitable for potent applications, such as in multilayer ceramic capacitors, devices for memory and high-density energy storage^[3]. In 2003, Kretly et al.^[4] successfully used CaCu₃Ti₄O₁₂ substrates for microwave devices and antennas. In 2004, Chung et al.^[5] observed highly non-ohmic current–voltage characteristics in CaCu₃Ti₄O₁₂ with nonlinear coefficient ≈ 912. This leads to the use of this material as an efficient switching (varistor-type device) and gas sensing device. In 2012, Felix et al.^[6] investigated thin films of CaCu₃Ti₄O₁₂ for potential applications, such as gas sensing, rectification, and resistive switching. In 2016, it was demonstrated that this material could serve as photocatalytic and photoelectrochemical materials with an excellent performance in visible light^[7]. Since then, pure and substituted CaCu₃Ti₄O₁₂ and related materials in monocrystalline, microcrystalline, nanophasic, nanocomposites, and thin-film forms have been extensively researched for potential use in a wide range of applications. In 2020, Chhetry et al.^[8] revealed a novel possibility for the easy design and development of superior CaCu₃Ti₄O₁₂ based capacitive sensors with versatile characteristics. Chattopadhyay et al.^[9] suggested the possible use of CaCu₃Ti₄O₁₂ nanopowder for application in a humidity sensor. Many research reports describing the fundamentals of experimental and theoretical researches on CaCu₃Ti₄O₁₂ based ceramic materials are available in the literature.

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 CaCu_2.95Cr_0.05Ti_4.1O₁₂ have been studied by Prompa et al.^[10]. The improvement of the breakdown field and the dielectric properties of Bi³⁺-Al³⁺ co-doped CaCu₃Ti₄O₁₂ have been investigated by Ren et al.^[11]. The dielectric properties, nonlinear electrical response, and microstructural evolution of CaCu₃Ti_4–xSn_xO₁₂ ceramics prepared by a double ball-milling process have been investigated by Boonlakhorn et al.^[12]. Cortes et al.^[13] performed dielectric and non-ohmic properties of Ca₂Cu₂Ti_4–xSn_xO₁₂ multiphasic ceramic composites. Comparative studies on pure and Sr²⁺ and Ni²⁺ doped and co-doped ceramics with special emphasis on the enhancement of dielectric properties have been published by Rhouma et al.^[14]. Wu et al.^[15] accomplished the effect of Ba²⁺ substitution on microstructure and electrical properties of Ca_1–xBa_xCu₃Ti₄O₁₂ ceramics. Enhanced nonlinear I–V response of Te⁴⁺ substituted CaCu₃Ti₄O₁₂ ceramics has been studied by Barman et al.^[16]. Meanwhile, the improvement in varistor properties of aliovalent Cr³⁺ substitution for Ti⁴⁺ in CaCu₃Ti_4–xCr_xO_12–δ series has been investigated by Grezebielucka et al.^[17]. Sun et al. studied improved dielectric properties of In³⁺ and Ta⁴⁺ co-substituted CaCu₃Ti₄O₁₂ ceramics prepared by spark plasma sintering^[18]. Very high-performance dielectric and non-ohmic properties of X and R-type Ca_1–1.5xHo_xCu₃Ti₄O₁₂/TiO₂ ceramics have been investigated by Sriakdee et al.^[19]. Finally, enhanced giant dielectric properties and improved electrical response in acceptor–donner (Al and Ta)-substituted CaCu₃Ti₄O₁₂ polycrystalline ceramics have been carried out by Boonlakhorn et al.^[20]. Unfortunately, these studies carry very limited and similar information, and were performed at T = 300 K. The same is the case with the thermal variation of dc electrical resistivity, ρ_dc (T), study. To the best of our knowledge, only a handful of research articles describing ρ_dc (T) characteristics of bulk^[21-24] and thin films^[25] of CaCu₃Ti₄O₁₂ are available in the literature. This gap has motivated us to carry out a systematic study of current density versus electric field characteristics over a wide temperature range and thermal variation of dc resistivity study of polycrystalline samples of quadruple perovskite series, CaCu_3–xTi_4–xFe_2xO₁₂ with x = 0.0, 0.1, 0.3, 0.5, and 0.7.

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 CaCu_3–xTi_4–xFe_2xO₁₂ 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, CaCu_3–xTi_4–xFe_2xO₁₂ with x = 0.0–0.7, in recent years (2018–2021)^[26-37]. In the system, divalent, weak magnetic (1 Bohr magneton), Jahn-Teller Cu²⁺ ions, and tetravalent, non-magnetic Ti⁴⁺ ions are simultaneously replaced by highly magnetic (5 Bohr magneton), trivalent Fe³⁺ ions in the series of quadruple perovskites, CaCu_3–xTi_4–xFe_2xO₁₂ where x varies from 0.0 to 0.7. Thus, interesting improvements in electrical behavior are expected. This work blends fundamental and applied research.

2. Experimental details

A series of cubic perovskites, CaCu_3–xTi_4–xFe_2xO₁₂ 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^{[27, 33]}. The measurements of current (I) versus applied signal voltage (V) (V = 0–400 V) (I–V characteristics) were carried out with the help of an Aplab made high-voltage dc regulated power supply (model no.׃ 7332) at temperatures ranging from T = 300–673 K using the two probe pressure contact method and a horizontal electric furnace. The cylindrically pelletized samples were rubbed with fine glass paper to give mirror-polished surfaces, and then cleaned with dilute hydrochloric acid and dimethyl ketone. To have perfect ohmic contact, microcracks on the surfaces were filled with a rubbing of graphite, and finally Al- foil was also kept on the surface. Instead of I–V characteristics, the traces of J versus E are taken into consideration, which eases the comparison between the I–V characteristics of the samples with varying thickness and surface area. A bi-terminal pressure contact method was employed to carry out the dc electrical resistivity measurement. The same set of the ceramic pellets, sample holder, vertical electric furnace, temperature indicator with thermocouple, and temperature controller used for thermal variation of I versus V characteristics was used to carry out temperature-dependent dc resistivity measurement. The resistance was directly measured using a mega-ohm meter supplied by BPL India. The thermal variation of resistance was obtained by keeping a sample holder containing a cylindrically pelletized sample in a horizontal electric furnace. For I–V characteristics and dc resistivity measurements as a function of temperature, an indigenously designed and fabricated sample holder was used. The holder consists of two ceramic beads with supporting metal roads. The spring-loaded brass electrode is introduced into the ceramic beads and pressed hard against the surface of the pellet. The second brass electrode is fixed at the other end. GELCO electronics private limited, India made PTS-7201 temperature indicator attached with K-type chromal-alumel thermocouple were used to measure the temperature of the pellet. The temperature of the furnace was controlled by maintaining the current passing through the heater employing a current controller (Bharat electrical Mumbai, India, made single phase auto-transformer). The resistance was noted during the cooling cycle at an interval of 20 °C in the temperature range of 300–773 K. A single set of temperature-dependent I–V characteristics and dc resistivity measurements have been performed.

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^[33]. The secondary phase is randomly distributed within the primary CaCu₃Ti₄O₁₂ matrix. Thus, Fe³⁺ substitution is restricted to x = 0.7 in the present study. In Tables 1 and 2, the structural and microstructural parameters are compiled to illustrate the compositional and temperature-dependent J–E characteristics.

Table 1. Structural, microstructural, and electric parameters for a series of cubic perovskites.

Fe^3+_ content (x)	Strain 10^–4	a (Å) ±0.002 Å	d_x (g/cm³)	d (g/cm³)	f	D (μm)	δ (10¹⁰m^–2)	T_sL (K)	E_s (V/cm) T = 473 K	J_max (mA/cm²)	E_a1 (eV)	E_a2 (eV)
0.0	–4.54	7.391	5.056	4.744	0.062	3.7	7.30	473	978	327	0.33	0.43
0.1	–6.16	7.388	5.061	4.712	0.069	–	–	373	570	270	0.29	0.29
0.3	–6.77	7.387	5.064	4.704	0.071	7.5	1.78	373	525	225	0.22	0.21
0.5	–5.96	7.400	5.038	4.556	0.096	7.9	1.60	373	261	225	0.25	0.15
0.7	–6.95	7.411	5.016	4.566	0.090	3.4	8.65	373	300	225	0.27	0.21
T_sL is the lowest temperature at which switching action takes place. E_s is the threshold value of the electric field beyond which non-ohmic behavior is observed. J_max is the maximum current density value. E_a1 and E_a2 are the activation energies determined from Arrhenius plots below and above the transition temperature, respectively.

DownLoad: CSV | Show Table

Table 2. Distribution of metallic cations (Ca⁺², Cu⁺², Ti⁺⁴ and Fe⁺³) among the available crystallographic sites determined from Rietvield refinement of X-ray powder diffraction data ( T = 300 K) for CaCu_3–xTi₄Fe_2xO₁₂ ( x = 0.0–0.7) system.

Fe³⁺ content (x)	Cation distribution
0.0	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{3}^{2+}$ ] { ${\mathrm{T}\mathrm{i}}_{4}^{4+}$ } ${\mathrm{O}}_{12}^{2-}$
0.1	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.86}^{2+}{\mathrm{F}\mathrm{e}}_{0.14}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.90}^{4+}{\mathrm{F}\mathrm{e}}_{0.06}^{3+}{\mathrm{C}\mathrm{u}}_{0.04}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.3	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.41}^{2+}{\mathrm{T}\mathrm{i}}_{0.24}^{4+}{\mathrm{F}\mathrm{e}}_{0.35}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.46}^{4+}{\mathrm{F}\mathrm{e}}_{0.25}^{3+}{\mathrm{C}\mathrm{u}}_{0.29}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.5	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.03}^{2+}{\mathrm{T}\mathrm{i}}_{0.17}^{4+}{\mathrm{F}\mathrm{e}}_{0.80}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.33}^{4+}{\mathrm{F}\mathrm{e}}_{0.20}^{3+}{\mathrm{C}\mathrm{u}}_{0.47}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.7	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{1.53}^{2+}{\mathrm{T}\mathrm{i}}_{0.12}^{4+}{\mathrm{F}\mathrm{e}}_{1.35}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.18}^{4+}{\mathrm{F}\mathrm{e}}_{0.05}^{3+}{\mathrm{C}\mathrm{u}}_{0.77}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$

DownLoad: CSV | Show Table

Fig. 1 gives the plots of J against E registered at different temperatures ranging from T = 300–773 K for the series CaCu_3–xTi_4–xFe_2xO₁₂. 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 (E_s) (E > E_s). 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 (T_sL) 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, E_s decreases with x for x = 0.0 to 0.5 compositions, while for x = 0.7 composition E_s shows small enhancement (Table 1). The compositional variation of E_s 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^[38]. The negative slope for all of the compositions suggests that a compressive strain has been produced (Fig. 2). The strain increases from –4.54 × 10^–4 for x = 0.0 composition to –6.77 × 10^–4 for x = 0.3 composition, it then decreases to –5.96 × 10^–4 for x = 0.5 composition and further increases to –6.95 × 10^–4 for x = 0.7 composition. It has been reported elsewhere that strain is directly proportional to T_sL and E_s, values^[26] but no such correlation has been observed in this work. Hu et al.^[39] have shown that for ceramically prepared compositions, E_s is inversely proportional to aggregate grain size (D) (E_s $\propto$ 1/D). For the series under investigation, D increases from 3.7 μm for x = 0.0 composition to 7.9 μm for x = 0.5 composition and then abruptly decreases to 3.4 μm for x = 0.7 composition^[33]. The increase of D means that there is a decrease in the number of grain-boundary barriers. Accordingly, E_s decreases from 978 V/cm for x = 0.0 composition to 261 V/cm for x = 0.5 composition and then for x = 0.7 composition E_s slightly increases to 300 V/cm, as shown in Table 1. Furthermore, observed decrease in T_sL and E_s for x = 0.0 – 0.3 compositions may be correlated with a subsequent decrease in lattice parameter (a (Å))^[38] (Table 1). The observed decrease in a with Fe-substitution (x) for the composition x = 0.0–0.3 infers that charge carriers need a small amount of energy for the conduction and thus T_sL and E_s decrease for x = 0.0–0.3 compositions. The observed dependence of E_s with Fe- content (x) can also be explained based on defects that occur during the sintering process. There are three types of defects: vacancy, dislocation, and grain boundary. The presence of these defects effectively modifies the material’s optical and electrical properties. It has been reported that interface defect density or dislocation density on grain boundaries (δ) $\propto$ 1/D² $\propto$ E_s² ^[26,38]. Thus, on increasing grain size from x = 0.0–0.5 compositions and observed grain size reduction for x = 0.7 composition turned into decrease in δ and E_svalues (x = 0.0–0.5) and increase in δ and E_svalues for x = 0.7 composition as observed (Table 1). The concentration of vacancy defects (C_d) determined from highly sophisticated PAL spectroscopy measurements^[29] decreases rapidly within the crystallites for x = 0.0–0.3 compositions and then saturates gradually for x = 0.5 and 0.7 compositions. The variation of C_d is consistent with the variation of E_s with Fe³⁺-content (x). This leads to a very important conclusion that the E_s is mainly controlled by C_d and δ.

Figure 1. (Color online) Plots of J–E characteristic recorded at different temperatures for a series of cubic perovskites, CaCu_3–xTi_4–xFe_2xO₁₂ (x = 0.0–0.7).

DownLoad: Full-Size Img PowerPoint

Figure 2. Williamson-Hall plots for all the samples of a series CaCu_3–xTi_4–xFe_2xO₁₂.

DownLoad: Full-Size Img PowerPoint

Another interesting observation from Fig. 1 is that maximum current density (J_max) 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, J_max 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 J_max. Zheng et al.^[40], following the density functional theory, have shown that in CaCu₃Ti₄O₁₂ the conduction mechanism is an adiabatic hopping conduction of small polarons and electron transport among CuO₄ square-planar (A´-site) clusters. Furthermore, the conduction band is chiefly contributed by the antibonding states of Cu 3d electrons. Usually, metal oxide series containing Jahn-Teller ions (high-spin d⁴ Cr²⁺ and Mn³⁺ ions, low-spin d⁷ Co²⁺ and d⁹ Cu²⁺ ions) are referred to as the most likely candidates to demonstrate switching action. Based on the above findings, it is clear that cupric ions on the A´-site play a governing role in switching phenomenon and electric conduction. It is now feasible to elucidate the compositional variation of J_max. The occupancy of metallic cations such as Ca²⁺, Cu²⁺, Ti⁴⁺ and Fe³⁺ among the crystallographic interstitial sites determined from Rietveld refinement of X-ray diffraction patterns revealed that with Fe- substitution the Cu²⁺-ion concentration at the A´ decreases from 3.0 for x = 0.0 composition to 1.53 for x = 0.7 composition^{[29, 33]}, as displayed in Table 2. This results in the curtailment of electric conduction through the square-planar site, and thus J_max decreases rapidly for x = 0.0–0.3 compositions and then levels off for the compositions with x = 0.5 and 0.7, as shown in Table 1. The observed reduction in J_max for x = 0.7 composition can also be explained based on the formation of a minor secondary insulating TiO₂-phase and reduced grain size. The percentage formation of these secondary phases is well below the theoretical percolation threshold (~16%) and experimental percolation threshold (~20%) values. This would ensure that electric behavior such as E_s and J_max would always be dominated by the CaCu₃Ti₄O₁₂ phase^[33]. An effort has been undertaken to correlate the previous outcome of the PAL spectroscopy study^[29] and present electric parameters as a function of composition (x). The magnitude of defect-specific positron lifetime (τ₂) reflects the contributions from the grain boundaries, vacancies, and vacancy clusters in grains. Earlier, it was found that τ₂ gradually increases from 0.2317 ns for x = 0.0 composition to 0.4449 ns for x = 0.5 composition and then level off for x = 0.7 composition to 0.4379 ns. The subsequent increase in τ₂ suggests that the thickness of grain-boundary layers increases with Fe-substitution for x = 0.0–0.5 compositions and saturate for x = 0.7 compositions. This limits the conduction of charge carriers from one conducting grain to the adjacent conducting grain separated by the highly resistive grain boundary. This is thought to be the cause of the observed initial reduction of J_max with x. On the same line of argument, E_s is expected to increase with x but no such trend has been observed. This suggests that as far as E_s value is concerned, an increase in grain size and decrease in defect density in grains dominant over the grain boundary broadening with Fe³⁺- substitution in the system, CaCu_3–xTi_4–xFe_2xO_12.

To the best of our knowledge, these values of J_max for the pure and Fe-substituted CaCu₃Ti₄O₁₂ ceramics are the highest ever reported values, except for those reported for Nb⁵⁺ and Ta⁵⁺-substituted CaCu₃Ti₄O₁₂ (J_max ≈ 275 mA/cm²)^[41]. Earlier, we have found J_max = 254 mA/cm² and 234 mA/cm² for quenched and microwave-assisted samples of CaCu₃Ti₄O₁₂, respectively^[26]. The nanocrystalline and microcrystalline samples of CaCu₃Ti₄O₁₂ synthesized by distinct routes (solid-state reaction, sol-gel, modified sol-gel, thermal decomposition, spark plasma sintering etc.) and treated with different conditions (atmoshphere, sintering temperature and duration etc.) have shown that J_max varies from 0.1–32 mA/cm²^{[3, 42-48]}. Meanwhile, Y and Mg co-doped samples of CaCu₃Ti₄O₁₂ have shown J_max ≈ 28 mA/cm²^[49], Sr-Ni substituted CaCu₃Ti₄O₁₂ have exhibited J_max ≈ 15 mA/cm²^[14], Pr-substituted CaCu₃Ti₄O₁₂ have demonstrated J_max = 15 mA/cm²^[50], while Zn + Zr co-doped CaCu₃Ti₄O₁₂ thin films show J_max in the range of 5–6 mA/cm²^[51]. Finally, the composites, (1–x) (CaCu₃Ti₄O₁₂)–(x)(0.1 Na_0.5 Bi_0.5TiO₃–0.9 BaTiO₃) with x = 0.02, 0.04, 0.06, 0.08 and 0.10, have shown J_max ranging from 13–20 mA/cm²^[52].

The existence of the Schottky barrier at the grain boundaries is signified by the observed linear relationship for ln J against E^1/2 traces^[53–55] (Fig. 3). The Schottky barrier height (ϕ_B) values determined from the slopes of the fitting lines of ln J₀ (J₀ is the value of J extrapolated to E = 0 V/cm) against reciprocal of temperature 1000/T graphs (Fig. 4) decreases from 0.25 eV for x = 0.0 composition to 0.21 eV for x = 0.5 composition while ϕ_B value increases to 0.28 eV for x = 0.7 compositions. The electric potential barrier height for the pristine composition, CaCu₃Ti₄O₁₂ is consistent with the reported value^[56]. Huang et al.^[54] have shown that the ϕ_B is influenced by the residual impurities and impurities from decomposition. The ϕ_B demonstrates a close linear relationship to the microstrain and δ.

Figure 3. (Color online) ln J against E^1/2 plots at different temperatures for polycrystalline samples of quadruple perovskite series, CaCu_3–xTi_4–xFe_2xO₁₂.

DownLoad: Full-Size Img PowerPoint

Figure 4. (Color online) Plots of ln J_o against temperature for the different compositions.

DownLoad: Full-Size Img PowerPoint

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^[57].

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 E_s) 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 E_s. 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 ( $\alpha$ ) is defined by the standard relation: α = (log J₂ – log J₁) / (log E₂ – log E₁), where J₁ and J₂ are calculated analogous to I₁ = 1 mA and I₂ = 10 mA, respectively, and E₁ and E₂ are the corresponding values of the electric fields. The electric field (E) and threshold voltage (E_s) decrease with increasing Fe³⁺-substitution (x) in the system, CaCu_3–xTi_4–xFe_2xO₁₂, for x = 0.0–0.5 compositions. This is attributed to the decrease of the number of grain boundaries due to the increase of average grain size^[58] from 3.7 μm for x = 0.0 composition to 7.9 μm for x = 0.5 composition, as depicted in Table 1. Meanwhile, with an increase in temperature and the concentration of highly magnetic Fe³⁺-ions (5μ_B) for non-magnetic Ti⁴⁺ (0 μ_B) in the system, the degree of Fe³⁺ + e^- → Fe²⁺ conduction that occurs on the square-planar site of the cubic perovskite structure is enhanced. Thus, I and J are expected to increase. These combined effects result in an increase in the value of α with temperature and Fe³⁺-substitution (x). The ranges of α value advise that these perovskites are best suited for low-voltage varistor applications. In the literature, a wide range of α values ranging from α = 1.91 to α = 912 have been reported for pristine composition, CaCu₃Ti₄O₁₂, registered at different temperatures, and synthesized with different sintering temperatures, preparative parameters, preparation routes, thermal history, voltage rise time in bulk, nanocrystalline and thin-film forms^[26].

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 (d_x) 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 (ρ_dc) for the different compositions have been determined from the experimental values of dc resistivity (ρ_p) recorded at different temperatures and void fraction values (f = 1 – (d/d_x)) with the help of the following relation ^[59] ׃

$ρ_{\rm{dc}} = ρ_{\rm p} \left[1 + f (1+ f ^{2/3})^{-1}\right]^{-1 },$

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 ρ_dc 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^[60] or may be associated with high-temperature structural phase transition reported occurring between T = 726–732 K for pure CaCu₃Ti₄O₁₂ composition^[61]. The activation energy values (E_a1and E_a2) were calculated for regions below and above the transition temperature, respectively, from the well-known Arrhenius equation and are shown in Table 1. In the low-temperature region, T = 300–573 K, E_a1 decreases from 0.33 eV for x = 0.0 composition to 0.22 eV for x = 0.3 composition, and then increases to 0.25 and 0.27 eV for x = 0.5 and 0.7 compositions, respectively. The lattice constant (a) value decreases from 7.391 Å for x = 0.0 composition to 7.387 Å for x = 0.3 composition, and then increases to 7.400 and 7.411 Å for x = 0.5 and 0.7 compositions, respectively (Table 1). The observed reduction in a with x suggests a corresponding decrease in interionic distances and as a result a decrease in barrier height encountered by the hopping charge carriers. Thus, E_a1 is supposed to decrease for x = 0.0–0.3 compositions. The same argument is applicable for the observed increase in E_a1 with an increase in a for x = 0.5 and 0.7 compositions. The average size of grains (D) also affects E_a1^[62]. A bigger grain size insinuates increased grain-to-grain contact area for the charge carrier to flow and consequently a lower barrier height, and vice versa. As discussed above, D increases from 3.7 μm for x = 0.0 composition to 7.9 μm for x = 0.5 composition and then decrease to 3.4 μm for x = 0.7 composition. This explains the observed dependence of E_a1 with Fe-content (x). The E_a1 values ranging from 0.22–0.33 eV are much higher than the ionization energy of acceptors and donors (i.e., 0.1 eV), and thus band-type conduction may not be possible. These values lie between the activation energy of a small polaron (≥ 0.5 eV) and the energy needed for the electron hopping mechanism (0.2 eV). Thus, the conduction proceeds by electrons with deformation. The E_a2 for the high-temperature regime are 0.43, 0.29, 0.21, 0.15, 0.21 eV, respectively, for x = 0.0, 0.1, 0.3, 0.5 and 0.7 compositions. Commonly, the resistivity of oxide ceramics is essentially dependent on the mobility and concentration of the carrier, but at such relatively low temperature it cannot be ascribed to oxygen depletion or absorption. The observed high-temperature deviation may be the result of the vacancy-disorder transition. Oxygen vacancies become ordered in the low-temperature regime, considerably enhancing the resistivity and thus higher activation energy. In the high-temperature regime, the conduction process is contributed by the oxygen ions and the oxygen vacancies are disordered, which allows oxygen ions to migrate with lower activation energy^[25]. Furthermore, in the temperature range studied, resistivity decreases with Fe³⁺-concentration (x). The incorporation of highly magnetic Fe³⁺ ions which take part in the process of conduction, for non-magnetic Ti⁴⁺ ions, enhances the degree of Fe³⁺ + e^– = Fe²⁺ conduction that occurs on the A´ - site of the cubic perovskite structure. Thus, dc resistivity decreases with Fe³⁺-substitution.

Figure 5. (Color online) Arrhenius plots for a quadruple perovskite series, CaCu_3–xTi_4–xFe_2x O₁₂.

DownLoad: Full-Size Img PowerPoint

4. Conclusions

The following conclusions can be drawn based on the electrical properties studies of a series of quadruple perovskites, CaCu_3–xTi_4–xFe_2xO₁₂ 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 J_max 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).

References

[1]	Subramanian M A, Li D, Duan N, et al. High dielectric constant in ACu₃Ti₄O₁₂ and ACu₃Ti₃FeO₁₂ phases. J Solid State Chem, 2000, 151, 323 doi: 10.1006/jssc.2000.8703
[2]	Ramirez A P, Subramanian M A, Gardel M, et al. Giant dielectric constant response in a copper-titanate. Solid State Commun, 2000, 115, 217 doi: 10.1016/S0038-1098(00)00182-4
[3]	Prompa K, Swatsitang E, Saiyasombat C, et al. Very high performance dielectric and non-Ohmics properties of CaCu₃Ti_4.₂O₁₂ ceramics for X8R capacitors. Ceram Int, 2018, 44, 13267 doi: 10.1016/j.ceramint.2018.04.156
[4]	Kretly L C, Almeida A F L, de Oliveira R S, et al. Electrical and optical properties of CaCu₃Ti₄O₁₂ (CCTO) substrates for microwave devices and antennas. Microw Opt Technol Lett, 2003, 39, 145 doi: 10.1002/mop.11152
[5]	Chung S Y, Kim I D, Kang S J L. Strong nonlinear current-voltage behaviour in perovskite-derivative calcium copper titanate. Nat Mater, 2004, 3, 774 doi: 10.1038/nmat1238
[6]	Felix A A, Rupp J L M, Varela J A, et al. Multi-functional properties of CaCu₃Ti₄O₁₂ thin films. J Appl Phys, 2012, 112, 054512 doi: 10.1063/1.4751344
[7]	Kushwaha H S, Madhar N A, Ilahi B, et al. Efficient solar energy conversion using CaCu₃Ti₄O₁₂ photoanode for photocatalysis and photoelectrocatalysis. Sci Rep, 2016, 6, 1 doi: 10.1038/s41598-016-0001-8
[8]	Chhetry A, Sharma S, Yoon H, et al. Enhanced sensitivity of capacitive pressure and strain sensor based on CaCu₃Ti₄O₁₂ wrapped hybrid sponge for wearable applications. Adv Funct Mater, 2020, 30, 1910020 doi: 10.1002/adfm.201910020
[9]	Chattopadhyay A, Nayak J. Synthesis of CCTO powder for application in humidity sensor. AIP Conference Proceedings, 2020, 040020
[10]	Prompa K, Swatsitang E, Putjuso T. Enhancement of nonlinear electrical properties with high performance dielectric properties of CaCu_2.₉₅Cr_0.₀₅Ti_4.₁O₁₂ ceramics. Ceram Int, 2018, 44, S72 doi: 10.1016/j.ceramint.2018.08.237
[11]	Ren L L, Yang L J, Xu C, et al. Improvement of breakdown field and dielectric properties of CaCu₃Ti₄O₁₂ ceramics by Bi and Al co-doping. J Alloys Compd, 2018, 768, 652 doi: 10.1016/j.jallcom.2018.07.293
[12]	Boonlakhorn J, Thongbai P. Dielectric properties, nonlinear electrical response and microstructural evolution of CaCu₃Ti_{4– x}Sn_xO₁₂ ceramics prepared by a double ball-milling process. Ceram Int, 2020, 46, 4952 doi: 10.1016/j.ceramint.2019.10.233
[13]	Cortés J A, Cotrim G, Orrego S, et al. Dielectric and non-ohmic properties of Ca₂Cu₂Ti_{4– x}Sn_xO₁₂ (0.0 ≤ x ≤ 4.0) multiphasic ceramic composites. J Alloys Compd, 2018, 735, 140 doi: 10.1016/j.jallcom.2017.11.089
[14]	Rhouma S, Saîd S, Autret C, et al. Comparative studies of pure, Sr-doped, Ni-doped and co-doped CaCu₃Ti₄O₁₂ ceramics: Enhancement of dielectric properties. J Alloys Compd, 2017, 717, 121 doi: 10.1016/j.jallcom.2017.05.053
[15]	Wu S, Liu P, Lai Y M, et al. Effect of Ba²⁺ doping on microstructure and electric properties of calcium copper titanate (CaCu₃Ti₄O₁₂) ceramics. J Mater Sci: Mater Electron, 2016, 27, 10336 doi: 10.1007/s10854-016-5118-9
[16]	Barman N, Varma K B R. Enhanced non-linear current-voltage response of Te-doped calcium copper titanate ceramics. Ceram Int, 2017, 43, 6363 doi: 10.1016/j.ceramint.2017.02.045
[17]	Grzebielucka E C, Leandro Monteiro J F H, de Souza E C F, et al. Improvement in varistor properties of CaCu₃Ti₄O₁₂ ceramics by chromium addition. J Mater Sci Technol, 2020, 41, 12 doi: 10.1016/j.jmst.2019.08.055
[18]	Sun J J, Xu C, Zhao X T, et al. Improved dielectric properties of indium and tantalum co-doped CaCu₃Ti₄O₁₂ ceramic prepared by spark plasma sintering. IEEE Trans Dielectr Electr Insul, 2020, 27, 1400 doi: 10.1109/TDEI.2020.008451
[19]	Sripakdee C, Prompa K, Swatsitang E, et al. Very high-performance dielectric and non-ohmic properties of novel X8R type Ca_{1–1.5 x}Ho_xCu₃Ti₄O₁₂/TiO₂ ceramics. J Alloys Compd, 2019, 779, 521 doi: 10.1016/j.jallcom.2018.11.298
[20]	Boonlakhorn J, Chanlek N, Manyam J, et al. Enhanced giant dielectric properties and improved nonlinear electrical response in acceptor-donor (Al³⁺, Ta⁵⁺)-substituted CaCu₃Ti₄O₁₂ ceramics. J Adv Ceram, 2021, 10, 1243 doi: 10.1007/s40145-021-0499-5
[21]	Löhnert R, Bartsch H, Schmidt R, et al. Microstructure and electric properties of CaCu₃Ti₄O₁₂ multilayer capacitors. J Am Ceram Soc, 2015, 98, 141 doi: 10.1111/jace.13260
[22]	Zheng Q, Fan H Q, Long C B. Microstructures and electrical responses of pure and chromium-doped CaCu₃Ti₄O₁₂ ceramics. J Alloys Compd, 2012, 511, 90 doi: 10.1016/j.jallcom.2011.09.002
[23]	Amhil S, Choukri E, Ben Moumen S, et al. Evidence of large hopping polaron conduction process in strontium doped calcium copper titanate ceramics. Phys B, 2019, 556, 36 doi: 10.1016/j.physb.2018.12.032
[24]	Fan H Q, Zheng Q, Peng B L. Microstructure, dielectric and pyroelectric properties of CaCu₃Ti₄O₁₂ ceramics fabricated by tape-casting method. Mater Res Bull, 2013, 48, 3278 doi: 10.1016/j.materresbull.2013.05.026
[25]	Chen L, Chen C L, Lin Y, et al. High temperature electrical properties of highly epitaxial CaCu₃Ti₄O₁₂ thin films on (001) LaAlO₃. Appl Phys Lett, 2003, 82, 2317 doi: 10.1063/1.1565702
[26]	Raval P Y, Makadiya A R, Pansara P R, et al. Effect of thermal history on structural, microstructural properties and J– E characteristics of CaCu₃Ti₄O₁₂ polycrystalline ceramic. Mater Chem Phys, 2018, 212, 343 doi: 10.1016/j.matchemphys.2018.03.041
[27]	Pansara P R, Raval P Y, Vasoya N H, et al. Intriguing structural and magnetic properties correlation study on Fe³⁺-substituted calcium-copper-titanate. Phys Chem Chem Phys, 2018, 20, 1914 doi: 10.1039/C7CP06681C
[28]	Raval P Y, Pansara P R, Vasoya N H, et al. Positron annihilation spectroscopic investigation of high energy ball - milling engendered defects in CaCu₃Ti₄O₁₂. Ceram Int, 2018, 44, 15887 doi: 10.1016/j.ceramint.2018.06.004
[29]	Pansara P R, Meshiya U M, Makadiya A R, et al. Defect structure transformation during substitution in quadruple perovskite CaCu_{3– x}Ti_{4– x}Fe_{2 x}O₁₂ studied by positron annihilation spectroscopy. Ceram Int, 2019, 45, 18599 doi: 10.1016/j.ceramint.2019.06.083
[30]	Raval P Y, Pansara P R, Makadiya A R, et al. Investigation on external stimuli engendered magnetic ordering in polycrystalline CaCu₃Ti₄O₁₂ quadruple perovskite. Ceram Int, 2018, 44, 17667 doi: 10.1016/j.ceramint.2018.06.230
[31]	Meshiya U M, Raval P Y, Pansara P R, et al. Electronic structure, orbital symmetry transformation, charge transfer, and valence state studies on Fe³⁺-substituted CaCu₃Ti₄O₁₂ quadruple perovskites using X-ray photoelectron spectroscopy. Ceram Int, 2020, 46, 2147 doi: 10.1016/j.ceramint.2019.09.198
[32]	Raval P Y, Pansara P R, Vasoya N H, et al. First observation of reversible mechanochromism and chromaticity study on calcium-copper-titanate. J Am Ceram Soc, 2019, 102, 6872 doi: 10.1111/jace.16609
[33]	Raval P Y, Joshi N P, Pansara P R, et al. A Ti L_{3, 2}- and K- edge XANES and EXAFS study on Fe³⁺-substituted CaCu₃Ti₄O₁₂. Ceram Int, 2018, 44, 20716 doi: 10.1016/j.ceramint.2018.08.066
[34]	Meshiya U M, Jani K K, Mange P L, et al. Defect characterization of slow-cooled and quenched samples of calcium-copper-titanate through positron annihilation spectroscopy. Spectrosc Lett, 2019, 52, 633 doi: 10.1080/00387010.2019.1681462
[35]	Pansara P R, Raval P Y, Pandit R, et al. First experimental evidence of non-collinear spin structure in CaCu_2.3Ti_3.3Fe_1.4O₁₂. Ceram Int, 2020, 46, 10016 doi: 10.1016/j.ceramint.2019.12.268
[36]	Meshiya U M, Raval P Y, Joshi N P, et al. Probing Fano resonance, relaxor ferroelectricity, light scattering by orbital exchange-bond, orbitons by Raman spectroscopy, and their correlation with dielectric properties of pure and Fe³⁺ - substituted calcium-copper-titanate. Vib Spectrosc, 2021, 112, 103201 doi: 10.1016/j.vibspec.2020.103201
[37]	Raval P Y, Pansara P R, Chen C L, et al. Probing reversal of orbital symmetry in CaCu_{3– x}Ti_{4– x}Fe_{2 x}O₁₂ (x = 0.0–0.7) by X-ray absorption spectroscopy. J Mater Sci: Mater Electron, 2021, 32, 13630 doi: 10.1007/s10854-021-05941-3
[38]	Modi K B, Vasoya N H, Pathak T K, et al. Observation of CCNR-type electrical switching in Zn_0.₃Mn_0.7_{+ x}Si_xFe_{2−2 x}O₄ spinel ferrite series. SN Appl Sci, 2020, 2, 1840 doi: 10.1007/s42452-020-03658-2
[39]	Hu W, Qin N, Wu G H, et al. Opportunity of spinel ferrite materials in nonvolatile memory device applications based on their resistive switching performances. J Am Chem Soc, 2012, 134, 14658 doi: 10.1021/ja305681n
[40]	Zheng P, Zhang R Z, Chen H Y, et al. Thermoelectric properties and conduction mechanism of CaCu₃Ti₄O₁₂ ceramics at high temperatures. J Electron Mater, 2014, 43, 1645 doi: 10.1007/s11664-013-2821-7
[41]	Chung S Y, Choi J H, Choi J K. Tunable current-voltage characteristics in polycrystalline calcium copper titanate. Appl Phys Lett, 2007, 91, 091912 doi: 10.1063/1.2777184
[42]	Mao P, Wang J P, Liu S J, et al. Grain size effect on the dielectric and non-ohmic properties of CaCu₃Ti₄O₁₂ ceramics prepared by the Sol-gel process. J Alloys Compd, 2019, 778, 625 doi: 10.1016/j.jallcom.2018.11.200
[43]	Zhao X T, Ren L L, Yang L J, et al. Structure and dielectric relaxations of CaCu₃Ti₄O₁₂ ceramics by heat treatments in different atmospheres. IEEE Trans Dielectr Electr Insul, 2017, 24, 764 doi: 10.1109/TDEI.2017.006278
[44]	Li T, He H F, Zhang T, et al. Effect of synthesizing temperatures on the microstructure and electrical property of CaCu₃Ti₄O₁₂ceramics prepared by sol-gel process. J Alloys Compd, 2016, 684, 315 doi: 10.1016/j.jallcom.2016.05.177
[45]	Putjuso S, Nunglek S, Putjuso T. Nonlinear current-voltage and dielectric properties of CaCu₃Ti₄O₁₂ ceramics prepared by an aloe vera solution method. RMUTSB Acad J, 2016, 4, 172
[46]	Kaur S, Kumar A, Sharma A L, et al. Dielectric and energy storage behavior of CaCu₃Ti₄O₁₂ nanoparticles for capacitor application. Ceram Int, 2019, 45, 7743 doi: 10.1016/j.ceramint.2019.01.077
[47]	Tang Z, Wu K N, Huang Y W, et al. High breakdown field CaCu₃Ti₄O₁₂ ceramics: Roles of the secondary phase and of Sr doping. Energies, 2017, 10, 1031 doi: 10.3390/en10071031
[48]	Lin H, He X, Gong Y Y, et al. Tuning the nonlinear current-voltage behavior of CaCu₃Ti₄O₁₂ ceramics by spark plasma sintering. Ceram Int, 2018, 44, 8650 doi: 10.1016/j.ceramint.2018.02.089
[49]	Boonlakhorn J, Putasaeng B, Kidkhunthod P, et al. Improved dielectric properties of (Y + Mg) co-doped CaCu₃Ti₄O₁₂ ceramics by controlling geometric and intrinsic properties of grain boundaries. Mater Des, 2016, 92, 494 doi: 10.1016/j.matdes.2015.12.042
[50]	Swatsitang E, Putjuso T. Very low loss tangent, high dielectric and non-ohmic properties of Ca_{1−1.5 x}Pr_xCu₃Ti₄O₁₂ ceramics prepared by the sol-gel process. J Mater Sci: Mater Electron, 2017, 28, 18966 doi: 10.1007/s10854-017-7850-1
[51]	Xu D, Yue X N, Song J, et al. Improved dielectric and non-ohmic properties of (Zn + Zr) codoped CaCu₃Ti₄O₁₂ thin films. Ceram Int, 2019, 45, 11421 doi: 10.1016/j.ceramint.2019.03.008
[52]	Mao P, Wang J P, Zhang L X, et al. Significantly enhanced breakdown field with high grain boundary resistance and dielectric response in 0.1Na_0.₅Bi_0.₅TiO₃-0.9BaTiO₃ doped CaCu₃Ti₄O₁₂ ceramics. J Eur Ceram Soc, 2020, 40, 3011 doi: 10.1016/j.jeurceramsoc.2020.03.032
[53]	Zang G Z, Zhang J L, Zheng P, et al. Grain boundary effect on the dielectric properties of CaCu₃Ti₄O₁₂ceramics. J Phys D, 2005, 38, 1824 doi: 10.1088/0022-3727/38/11/022
[54]	Huang Y M, Shi D P, Li Y H, et al. Effect of holding time on the dielectric properties and non-ohmic behavior of CaCu₃Ti₄O₁₂ capacitor-varistors. J Mater Sci: Mater Electron, 2013, 24, 1994 doi: 10.1007/s10854-012-1047-4
[55]	Xiao M, Wang K Y, Chenyang X Q, et al. Nonlinear current-voltage behavior of CaCu₃Ti₄O₁₂ thin films derived from Sol-gel method. J Mater Sci: Mater Electron, 2014, 25, 2710 doi: 10.1007/s10854-014-1933-z
[56]	Felix A A, Orlandi M O, Varela J A. Schottky-type grain boundaries in CCTO ceramics. Solid State Commun, 2011, 151, 1377 doi: 10.1016/j.ssc.2011.06.012
[57]	https://www.creativesaftysupply.com
[58]	Abdullah K A L, Termanini M D, Omar F A. Effect of impurities and temperature on electrical properties of ZnO-based varistors. Energy Procedia, 2012, 18, 867 doi: 10.1016/j.egypro.2012.05.101
[59]	Russell H W. Principles of heat flow in porous insulators. J Am Ceram Soc, 1935, 18, 1 doi: 10.1111/j.1151-2916.1935.tb19340.x
[60]	Onodera A, Takesada M, Kawatani K, et al. Dielectric properties and phase transition in CaCu₃Ti₄O₁₂ at high temperatures. Jpn J Appl Phys, 2008, 47, 7753 doi: 10.1143/JJAP.47.7753
[61]	Gorev M V, Flerov I N, Kartashev A V, et al. Investigation of the thermal expansion and heat capacity of the CaCu₃Ti₄O₁₂ ceramics. Phys Solid State, 2012, 54, 1785 doi: 10.1134/S1063783412090120
[62]	Lakhani V K, Modi K B. Effect of Al³⁺ substitution on the transport properties of copper ferrite. J Phys D, 2011, 44, 245403 doi: 10.1088/0022-3727/44/24/245403

Fig. 1. (Color online) Plots of J–E characteristic recorded at different temperatures for a series of cubic perovskites, CaCu_3–xTi_4–xFe_2xO₁₂ (x = 0.0–0.7).

DownLoad: Full-Size Img PowerPoint

Fig. 2. Williamson-Hall plots for all the samples of a series CaCu_3–xTi_4–xFe_2xO₁₂.

DownLoad: Full-Size Img PowerPoint

Fig. 3. (Color online) ln J against E^1/2 plots at different temperatures for polycrystalline samples of quadruple perovskite series, CaCu_3–xTi_4–xFe_2xO₁₂.

DownLoad: Full-Size Img PowerPoint

Fig. 4. (Color online) Plots of ln J_o against temperature for the different compositions.

DownLoad: Full-Size Img PowerPoint

Fig. 5. (Color online) Arrhenius plots for a quadruple perovskite series, CaCu_3–xTi_4–xFe_2x O₁₂.

DownLoad: Full-Size Img PowerPoint

Table 1. Structural, microstructural, and electric parameters for a series of cubic perovskites.

Fe^3+_ content (x)	Strain 10^–4	a (Å) ±0.002 Å	d_x (g/cm³)	d (g/cm³)	f	D (μm)	δ (10¹⁰m^–2)	T_sL (K)	E_s (V/cm) T = 473 K	J_max (mA/cm²)	E_a1 (eV)	E_a2 (eV)
0.0	–4.54	7.391	5.056	4.744	0.062	3.7	7.30	473	978	327	0.33	0.43
0.1	–6.16	7.388	5.061	4.712	0.069	–	–	373	570	270	0.29	0.29
0.3	–6.77	7.387	5.064	4.704	0.071	7.5	1.78	373	525	225	0.22	0.21
0.5	–5.96	7.400	5.038	4.556	0.096	7.9	1.60	373	261	225	0.25	0.15
0.7	–6.95	7.411	5.016	4.566	0.090	3.4	8.65	373	300	225	0.27	0.21
T_sL is the lowest temperature at which switching action takes place. E_s is the threshold value of the electric field beyond which non-ohmic behavior is observed. J_max is the maximum current density value. E_a1 and E_a2 are the activation energies determined from Arrhenius plots below and above the transition temperature, respectively.

DownLoad: CSV

Fe³⁺ content (x)	Cation distribution
0.0	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{3}^{2+}$ ] { ${\mathrm{T}\mathrm{i}}_{4}^{4+}$ } ${\mathrm{O}}_{12}^{2-}$
0.1	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.86}^{2+}{\mathrm{F}\mathrm{e}}_{0.14}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.90}^{4+}{\mathrm{F}\mathrm{e}}_{0.06}^{3+}{\mathrm{C}\mathrm{u}}_{0.04}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.3	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.41}^{2+}{\mathrm{T}\mathrm{i}}_{0.24}^{4+}{\mathrm{F}\mathrm{e}}_{0.35}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.46}^{4+}{\mathrm{F}\mathrm{e}}_{0.25}^{3+}{\mathrm{C}\mathrm{u}}_{0.29}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.5	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{2.03}^{2+}{\mathrm{T}\mathrm{i}}_{0.17}^{4+}{\mathrm{F}\mathrm{e}}_{0.80}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.33}^{4+}{\mathrm{F}\mathrm{e}}_{0.20}^{3+}{\mathrm{C}\mathrm{u}}_{0.47}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$
0.7	${\mathrm{C}\mathrm{a}}^{2+}$ [ ${\mathrm{C}\mathrm{u}}_{1.53}^{2+}{\mathrm{T}\mathrm{i}}_{0.12}^{4+}{\mathrm{F}\mathrm{e}}_{1.35}^{3+}$ ] { ${\mathrm{T}\mathrm{i}}_{3.18}^{4+}{\mathrm{F}\mathrm{e}}_{0.05}^{3+}{\mathrm{C}\mathrm{u}}_{0.77}^{2+}$ } ${\mathrm{O}}_{12}^{2-}$

DownLoad: CSV

[1]	Subramanian M A, Li D, Duan N, et al. High dielectric constant in ACu₃Ti₄O₁₂ and ACu₃Ti₃FeO₁₂ phases. J Solid State Chem, 2000, 151, 323 doi: 10.1006/jssc.2000.8703
[2]	Ramirez A P, Subramanian M A, Gardel M, et al. Giant dielectric constant response in a copper-titanate. Solid State Commun, 2000, 115, 217 doi: 10.1016/S0038-1098(00)00182-4
[3]	Prompa K, Swatsitang E, Saiyasombat C, et al. Very high performance dielectric and non-Ohmics properties of CaCu₃Ti_4.₂O₁₂ ceramics for X8R capacitors. Ceram Int, 2018, 44, 13267 doi: 10.1016/j.ceramint.2018.04.156
[4]	Kretly L C, Almeida A F L, de Oliveira R S, et al. Electrical and optical properties of CaCu₃Ti₄O₁₂ (CCTO) substrates for microwave devices and antennas. Microw Opt Technol Lett, 2003, 39, 145 doi: 10.1002/mop.11152
[5]	Chung S Y, Kim I D, Kang S J L. Strong nonlinear current-voltage behaviour in perovskite-derivative calcium copper titanate. Nat Mater, 2004, 3, 774 doi: 10.1038/nmat1238
[6]	Felix A A, Rupp J L M, Varela J A, et al. Multi-functional properties of CaCu₃Ti₄O₁₂ thin films. J Appl Phys, 2012, 112, 054512 doi: 10.1063/1.4751344
[7]	Kushwaha H S, Madhar N A, Ilahi B, et al. Efficient solar energy conversion using CaCu₃Ti₄O₁₂ photoanode for photocatalysis and photoelectrocatalysis. Sci Rep, 2016, 6, 1 doi: 10.1038/s41598-016-0001-8
[8]	Chhetry A, Sharma S, Yoon H, et al. Enhanced sensitivity of capacitive pressure and strain sensor based on CaCu₃Ti₄O₁₂ wrapped hybrid sponge for wearable applications. Adv Funct Mater, 2020, 30, 1910020 doi: 10.1002/adfm.201910020
[9]	Chattopadhyay A, Nayak J. Synthesis of CCTO powder for application in humidity sensor. AIP Conference Proceedings, 2020, 040020
[10]	Prompa K, Swatsitang E, Putjuso T. Enhancement of nonlinear electrical properties with high performance dielectric properties of CaCu_2.₉₅Cr_0.₀₅Ti_4.₁O₁₂ ceramics. Ceram Int, 2018, 44, S72 doi: 10.1016/j.ceramint.2018.08.237
[11]	Ren L L, Yang L J, Xu C, et al. Improvement of breakdown field and dielectric properties of CaCu₃Ti₄O₁₂ ceramics by Bi and Al co-doping. J Alloys Compd, 2018, 768, 652 doi: 10.1016/j.jallcom.2018.07.293
[12]	Boonlakhorn J, Thongbai P. Dielectric properties, nonlinear electrical response and microstructural evolution of CaCu₃Ti_{4– x}Sn_xO₁₂ ceramics prepared by a double ball-milling process. Ceram Int, 2020, 46, 4952 doi: 10.1016/j.ceramint.2019.10.233
[13]	Cortés J A, Cotrim G, Orrego S, et al. Dielectric and non-ohmic properties of Ca₂Cu₂Ti_{4– x}Sn_xO₁₂ (0.0 ≤ x ≤ 4.0) multiphasic ceramic composites. J Alloys Compd, 2018, 735, 140 doi: 10.1016/j.jallcom.2017.11.089
[14]	Rhouma S, Saîd S, Autret C, et al. Comparative studies of pure, Sr-doped, Ni-doped and co-doped CaCu₃Ti₄O₁₂ ceramics: Enhancement of dielectric properties. J Alloys Compd, 2017, 717, 121 doi: 10.1016/j.jallcom.2017.05.053
[15]	Wu S, Liu P, Lai Y M, et al. Effect of Ba²⁺ doping on microstructure and electric properties of calcium copper titanate (CaCu₃Ti₄O₁₂) ceramics. J Mater Sci: Mater Electron, 2016, 27, 10336 doi: 10.1007/s10854-016-5118-9
[16]	Barman N, Varma K B R. Enhanced non-linear current-voltage response of Te-doped calcium copper titanate ceramics. Ceram Int, 2017, 43, 6363 doi: 10.1016/j.ceramint.2017.02.045
[17]	Grzebielucka E C, Leandro Monteiro J F H, de Souza E C F, et al. Improvement in varistor properties of CaCu₃Ti₄O₁₂ ceramics by chromium addition. J Mater Sci Technol, 2020, 41, 12 doi: 10.1016/j.jmst.2019.08.055
[18]	Sun J J, Xu C, Zhao X T, et al. Improved dielectric properties of indium and tantalum co-doped CaCu₃Ti₄O₁₂ ceramic prepared by spark plasma sintering. IEEE Trans Dielectr Electr Insul, 2020, 27, 1400 doi: 10.1109/TDEI.2020.008451
[19]	Sripakdee C, Prompa K, Swatsitang E, et al. Very high-performance dielectric and non-ohmic properties of novel X8R type Ca_{1–1.5 x}Ho_xCu₃Ti₄O₁₂/TiO₂ ceramics. J Alloys Compd, 2019, 779, 521 doi: 10.1016/j.jallcom.2018.11.298
[20]	Boonlakhorn J, Chanlek N, Manyam J, et al. Enhanced giant dielectric properties and improved nonlinear electrical response in acceptor-donor (Al³⁺, Ta⁵⁺)-substituted CaCu₃Ti₄O₁₂ ceramics. J Adv Ceram, 2021, 10, 1243 doi: 10.1007/s40145-021-0499-5
[21]	Löhnert R, Bartsch H, Schmidt R, et al. Microstructure and electric properties of CaCu₃Ti₄O₁₂ multilayer capacitors. J Am Ceram Soc, 2015, 98, 141 doi: 10.1111/jace.13260
[22]	Zheng Q, Fan H Q, Long C B. Microstructures and electrical responses of pure and chromium-doped CaCu₃Ti₄O₁₂ ceramics. J Alloys Compd, 2012, 511, 90 doi: 10.1016/j.jallcom.2011.09.002
[23]	Amhil S, Choukri E, Ben Moumen S, et al. Evidence of large hopping polaron conduction process in strontium doped calcium copper titanate ceramics. Phys B, 2019, 556, 36 doi: 10.1016/j.physb.2018.12.032
[24]	Fan H Q, Zheng Q, Peng B L. Microstructure, dielectric and pyroelectric properties of CaCu₃Ti₄O₁₂ ceramics fabricated by tape-casting method. Mater Res Bull, 2013, 48, 3278 doi: 10.1016/j.materresbull.2013.05.026
[25]	Chen L, Chen C L, Lin Y, et al. High temperature electrical properties of highly epitaxial CaCu₃Ti₄O₁₂ thin films on (001) LaAlO₃. Appl Phys Lett, 2003, 82, 2317 doi: 10.1063/1.1565702
[26]	Raval P Y, Makadiya A R, Pansara P R, et al. Effect of thermal history on structural, microstructural properties and J– E characteristics of CaCu₃Ti₄O₁₂ polycrystalline ceramic. Mater Chem Phys, 2018, 212, 343 doi: 10.1016/j.matchemphys.2018.03.041
[27]	Pansara P R, Raval P Y, Vasoya N H, et al. Intriguing structural and magnetic properties correlation study on Fe³⁺-substituted calcium-copper-titanate. Phys Chem Chem Phys, 2018, 20, 1914 doi: 10.1039/C7CP06681C
[28]	Raval P Y, Pansara P R, Vasoya N H, et al. Positron annihilation spectroscopic investigation of high energy ball - milling engendered defects in CaCu₃Ti₄O₁₂. Ceram Int, 2018, 44, 15887 doi: 10.1016/j.ceramint.2018.06.004
[29]	Pansara P R, Meshiya U M, Makadiya A R, et al. Defect structure transformation during substitution in quadruple perovskite CaCu_{3– x}Ti_{4– x}Fe_{2 x}O₁₂ studied by positron annihilation spectroscopy. Ceram Int, 2019, 45, 18599 doi: 10.1016/j.ceramint.2019.06.083
[30]	Raval P Y, Pansara P R, Makadiya A R, et al. Investigation on external stimuli engendered magnetic ordering in polycrystalline CaCu₃Ti₄O₁₂ quadruple perovskite. Ceram Int, 2018, 44, 17667 doi: 10.1016/j.ceramint.2018.06.230
[31]	Meshiya U M, Raval P Y, Pansara P R, et al. Electronic structure, orbital symmetry transformation, charge transfer, and valence state studies on Fe³⁺-substituted CaCu₃Ti₄O₁₂ quadruple perovskites using X-ray photoelectron spectroscopy. Ceram Int, 2020, 46, 2147 doi: 10.1016/j.ceramint.2019.09.198
[32]	Raval P Y, Pansara P R, Vasoya N H, et al. First observation of reversible mechanochromism and chromaticity study on calcium-copper-titanate. J Am Ceram Soc, 2019, 102, 6872 doi: 10.1111/jace.16609
[33]	Raval P Y, Joshi N P, Pansara P R, et al. A Ti L_{3, 2}- and K- edge XANES and EXAFS study on Fe³⁺-substituted CaCu₃Ti₄O₁₂. Ceram Int, 2018, 44, 20716 doi: 10.1016/j.ceramint.2018.08.066
[34]	Meshiya U M, Jani K K, Mange P L, et al. Defect characterization of slow-cooled and quenched samples of calcium-copper-titanate through positron annihilation spectroscopy. Spectrosc Lett, 2019, 52, 633 doi: 10.1080/00387010.2019.1681462
[35]	Pansara P R, Raval P Y, Pandit R, et al. First experimental evidence of non-collinear spin structure in CaCu_2.3Ti_3.3Fe_1.4O₁₂. Ceram Int, 2020, 46, 10016 doi: 10.1016/j.ceramint.2019.12.268
[36]	Meshiya U M, Raval P Y, Joshi N P, et al. Probing Fano resonance, relaxor ferroelectricity, light scattering by orbital exchange-bond, orbitons by Raman spectroscopy, and their correlation with dielectric properties of pure and Fe³⁺ - substituted calcium-copper-titanate. Vib Spectrosc, 2021, 112, 103201 doi: 10.1016/j.vibspec.2020.103201
[37]	Raval P Y, Pansara P R, Chen C L, et al. Probing reversal of orbital symmetry in CaCu_{3– x}Ti_{4– x}Fe_{2 x}O₁₂ (x = 0.0–0.7) by X-ray absorption spectroscopy. J Mater Sci: Mater Electron, 2021, 32, 13630 doi: 10.1007/s10854-021-05941-3
[38]	Modi K B, Vasoya N H, Pathak T K, et al. Observation of CCNR-type electrical switching in Zn_0.₃Mn_0.7_{+ x}Si_xFe_{2−2 x}O₄ spinel ferrite series. SN Appl Sci, 2020, 2, 1840 doi: 10.1007/s42452-020-03658-2
[39]	Hu W, Qin N, Wu G H, et al. Opportunity of spinel ferrite materials in nonvolatile memory device applications based on their resistive switching performances. J Am Chem Soc, 2012, 134, 14658 doi: 10.1021/ja305681n
[40]	Zheng P, Zhang R Z, Chen H Y, et al. Thermoelectric properties and conduction mechanism of CaCu₃Ti₄O₁₂ ceramics at high temperatures. J Electron Mater, 2014, 43, 1645 doi: 10.1007/s11664-013-2821-7
[41]	Chung S Y, Choi J H, Choi J K. Tunable current-voltage characteristics in polycrystalline calcium copper titanate. Appl Phys Lett, 2007, 91, 091912 doi: 10.1063/1.2777184
[42]	Mao P, Wang J P, Liu S J, et al. Grain size effect on the dielectric and non-ohmic properties of CaCu₃Ti₄O₁₂ ceramics prepared by the Sol-gel process. J Alloys Compd, 2019, 778, 625 doi: 10.1016/j.jallcom.2018.11.200
[43]	Zhao X T, Ren L L, Yang L J, et al. Structure and dielectric relaxations of CaCu₃Ti₄O₁₂ ceramics by heat treatments in different atmospheres. IEEE Trans Dielectr Electr Insul, 2017, 24, 764 doi: 10.1109/TDEI.2017.006278
[44]	Li T, He H F, Zhang T, et al. Effect of synthesizing temperatures on the microstructure and electrical property of CaCu₃Ti₄O₁₂ceramics prepared by sol-gel process. J Alloys Compd, 2016, 684, 315 doi: 10.1016/j.jallcom.2016.05.177
[45]	Putjuso S, Nunglek S, Putjuso T. Nonlinear current-voltage and dielectric properties of CaCu₃Ti₄O₁₂ ceramics prepared by an aloe vera solution method. RMUTSB Acad J, 2016, 4, 172
[46]	Kaur S, Kumar A, Sharma A L, et al. Dielectric and energy storage behavior of CaCu₃Ti₄O₁₂ nanoparticles for capacitor application. Ceram Int, 2019, 45, 7743 doi: 10.1016/j.ceramint.2019.01.077
[47]	Tang Z, Wu K N, Huang Y W, et al. High breakdown field CaCu₃Ti₄O₁₂ ceramics: Roles of the secondary phase and of Sr doping. Energies, 2017, 10, 1031 doi: 10.3390/en10071031
[48]	Lin H, He X, Gong Y Y, et al. Tuning the nonlinear current-voltage behavior of CaCu₃Ti₄O₁₂ ceramics by spark plasma sintering. Ceram Int, 2018, 44, 8650 doi: 10.1016/j.ceramint.2018.02.089
[49]	Boonlakhorn J, Putasaeng B, Kidkhunthod P, et al. Improved dielectric properties of (Y + Mg) co-doped CaCu₃Ti₄O₁₂ ceramics by controlling geometric and intrinsic properties of grain boundaries. Mater Des, 2016, 92, 494 doi: 10.1016/j.matdes.2015.12.042
[50]	Swatsitang E, Putjuso T. Very low loss tangent, high dielectric and non-ohmic properties of Ca_{1−1.5 x}Pr_xCu₃Ti₄O₁₂ ceramics prepared by the sol-gel process. J Mater Sci: Mater Electron, 2017, 28, 18966 doi: 10.1007/s10854-017-7850-1
[51]	Xu D, Yue X N, Song J, et al. Improved dielectric and non-ohmic properties of (Zn + Zr) codoped CaCu₃Ti₄O₁₂ thin films. Ceram Int, 2019, 45, 11421 doi: 10.1016/j.ceramint.2019.03.008
[52]	Mao P, Wang J P, Zhang L X, et al. Significantly enhanced breakdown field with high grain boundary resistance and dielectric response in 0.1Na_0.₅Bi_0.₅TiO₃-0.9BaTiO₃ doped CaCu₃Ti₄O₁₂ ceramics. J Eur Ceram Soc, 2020, 40, 3011 doi: 10.1016/j.jeurceramsoc.2020.03.032
[53]	Zang G Z, Zhang J L, Zheng P, et al. Grain boundary effect on the dielectric properties of CaCu₃Ti₄O₁₂ceramics. J Phys D, 2005, 38, 1824 doi: 10.1088/0022-3727/38/11/022
[54]	Huang Y M, Shi D P, Li Y H, et al. Effect of holding time on the dielectric properties and non-ohmic behavior of CaCu₃Ti₄O₁₂ capacitor-varistors. J Mater Sci: Mater Electron, 2013, 24, 1994 doi: 10.1007/s10854-012-1047-4
[55]	Xiao M, Wang K Y, Chenyang X Q, et al. Nonlinear current-voltage behavior of CaCu₃Ti₄O₁₂ thin films derived from Sol-gel method. J Mater Sci: Mater Electron, 2014, 25, 2710 doi: 10.1007/s10854-014-1933-z
[56]	Felix A A, Orlandi M O, Varela J A. Schottky-type grain boundaries in CCTO ceramics. Solid State Commun, 2011, 151, 1377 doi: 10.1016/j.ssc.2011.06.012
[57]	https://www.creativesaftysupply.com
[58]	Abdullah K A L, Termanini M D, Omar F A. Effect of impurities and temperature on electrical properties of ZnO-based varistors. Energy Procedia, 2012, 18, 867 doi: 10.1016/j.egypro.2012.05.101
[59]	Russell H W. Principles of heat flow in porous insulators. J Am Ceram Soc, 1935, 18, 1 doi: 10.1111/j.1151-2916.1935.tb19340.x
[60]	Onodera A, Takesada M, Kawatani K, et al. Dielectric properties and phase transition in CaCu₃Ti₄O₁₂ at high temperatures. Jpn J Appl Phys, 2008, 47, 7753 doi: 10.1143/JJAP.47.7753
[61]	Gorev M V, Flerov I N, Kartashev A V, et al. Investigation of the thermal expansion and heat capacity of the CaCu₃Ti₄O₁₂ ceramics. Phys Solid State, 2012, 54, 1785 doi: 10.1134/S1063783412090120
[62]	Lakhani V K, Modi K B. Effect of Al³⁺ substitution on the transport properties of copper ferrite. J Phys D, 2011, 44, 245403 doi: 10.1088/0022-3727/44/24/245403

1	Advances in perovskite lasers Zhicheng Guan, Hengyu Zhang, Guang Yang Journal of Semiconductors, 2025, 46(4): 041401. doi: 10.1088/1674-4926/24100029
2	Observation of exciton polariton condensation in a perovskite lattice at room temperature Jun Zhang Journal of Semiconductors, 2020, 41(3): 030201. doi: 10.1088/1674-4926/41/3/030201
3	A compact two-dimensional analytical model of the electrical characteristics of a triple-material double-gate tunneling FET structure C. Usha, P. Vimala Journal of Semiconductors, 2019, 40(12): 122901. doi: 10.1088/1674-4926/40/12/122901
4	Perovskite plasmonic lasers capable of mode modulation Jingbi You Journal of Semiconductors, 2019, 40(7): 070203. doi: 10.1088/1674-4926/40/7/070203
5	Surface passivation of perovskite film for efficient solar cells Yang (Michael) Yang Journal of Semiconductors, 2019, 40(4): 040204. doi: 10.1088/1674-4926/40/4/040204
6	Analytical model for the effects of the variation of ferrolectric material parameters on the minimum subthreshold swing in negative capacitance capacitor Raheela Rasool, Najeeb-ud-Din, G. M. Rather Journal of Semiconductors, 2019, 40(12): 122401. doi: 10.1088/1674-4926/40/12/122401
7	Flexible devices: from materials, architectures to applications Mingzhi Zou, Yue Ma, Xin Yuan, Yi Hu, Jie Liu, et al. Journal of Semiconductors, 2018, 39(1): 011010. doi: 10.1088/1674-4926/39/1/011010
8	Fabrication and modeling of multi-layer metal–insulator-metal capacitors R Karthik, A Akshaykranth Journal of Semiconductors, 2017, 38(12): 123002. doi: 10.1088/1674-4926/38/12/123002
9	Improved interfacial properties of GaAs MOS capacitor with NH₃-plasma-treated ZnON as interfacial passivation layer Jingkang Gong, Jingping Xu, Lu Liu, Hanhan Lu, Xiaoyu Liu, et al. Journal of Semiconductors, 2017, 38(9): 094004. doi: 10.1088/1674-4926/38/9/094004
10	Research progress of Si-based germanium materials and devices Buwen Cheng, Cheng Li, Zhi Liu, Chunlai Xue Journal of Semiconductors, 2016, 37(8): 081001. doi: 10.1088/1674-4926/37/8/081001
11	Pb(Zr_0.52Ti_0.48)O₃ memory capacitor on Si with a polycrystalline silicon/SiO₂ stacked buffer layer Cai Daolin, Li Ping, Zhai Yahong, Song Zhitang, Chen Houpeng, et al. Journal of Semiconductors, 2011, 32(9): 094007. doi: 10.1088/1674-4926/32/9/094007
12	Low-power switched-capacitor delta-sigma modulator for EEG recording applications Chen Jin, Zhang Xu, Chen Hongda Journal of Semiconductors, 2010, 31(7): 075009. doi: 10.1088/1674-4926/31/7/075009
13	A low-power and low-phase-noise LC digitally controlled oscillator featuring a novel capacitor bank Tian Huanhuan, Li Zhiqiang, Chen Pufeng, Wu Rufei, Zhang Haiying, et al. Journal of Semiconductors, 2010, 31(12): 125003. doi: 10.1088/1674-4926/31/12/125003
14	Design of an LDO with capacitor multiplier Ying Jianhua, Huang Meng, Huang Yang Journal of Semiconductors, 2010, 31(7): 075010. doi: 10.1088/1674-4926/31/7/075010
15	TDDB improvement by optimized processes on metal–insulator–silicon capacitors with atomic layer deposition of Al2O3 and multi layers of TiN film structure Peng Kun, Wang Biao, Xiao Deyuan, Qiu Shengfen, Lin D C, et al. Journal of Semiconductors, 2009, 30(8): 082005. doi: 10.1088/1674-4926/30/8/082005
16	An offset-insensitive switched-capacitor bandgap reference with continuous output Zheng Peng, Yan Wei, Zhang Ke, Li Wenhong Journal of Semiconductors, 2009, 30(8): 085006. doi: 10.1088/1674-4926/30/8/085006
17	Capacitance–voltage characterization of fully silicided gated MOS capacitor Wang Baomin, Ru Guoping, Jiang Yulong, Qu Xinping, Li Bingzong, et al. Journal of Semiconductors, 2009, 30(3): 034002. doi: 10.1088/1674-4926/30/3/034002
18	MMIC-Based RF On-Chip LC Passive Filters Wu Rui, Liao Xiaoping, Zhang Zhiqiang Journal of Semiconductors, 2008, 29(12): 2437-2442.
19	Status and Trends in Advanced SOI Devices and Materials Balestra Francis Chinese Journal of Semiconductors , 2006, 27(4): 573-582.
20	Status and Trends in Advanced SOI Devices and Materials Wang Tianxing, Wei Hongxiang, Ren Cong, Han Xiufeng, Clifford E, et al. Chinese Journal of Semiconductors , 2006, 27(4): 591-597.

1.	Parekh, D.J., Meshiya, U.M., Raval, P.Y. et al. Influence of Fe3+ substitution on crystallographic and magnetic structures of CaCu3Ti4O12 perovskites: powder X-ray and neutron diffraction studies. Journal of Materials Science: Materials in Electronics, 2024, 35(32): 2051. doi:10.1007/s10854-024-13766-z
2.	Parekh, D.J., Barad, D.V., Thummar, D.K. et al. Influence of Ca2+ Substitution on Elastic Properties of CaCu3Ti4O12 Quadruple Perovskites Determined by Ultrasonic Pulse Echo Selection Technique. Russian Journal of Nondestructive Testing, 2024, 60(6): 614-635. doi:10.1134/S1061830924601545

Search

GET CITATION

Kunal B. Modi, Pooja Y. Raval, Dolly J. Parekh, Shrey K. Modi, Niketa P. Joshi, Akshay R. Makadiya, Nimish H. Vasoya, Utpal S. Joshi. Fe³⁺-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu₃Ti₄O₁₂[J]. Journal of Semiconductors, 2022, 43(3): 032001. doi: 10.1088/1674-4926/43/3/032001

K B Modi, P Y Raval, D J Parekh, S K Modi, N P Joshi, A R Makadiya, N H Vasoya, U S Joshi, Fe3+-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu3Ti4O12[J]. J. Semicond., 2022, 43(3): 032001. doi: 10.1088/1674-4926/43/3/032001.

Export: BibTex EndNote

Article Metrics

Article views: 1764 Times PDF downloads: 62 Times Cited by: 2 Times

History

Received: 15 September 2021 Revised: 19 November 2021 Online: Uncorrected proof: 31 December 2021Published: 10 March 2022

Article Navigation > Journal of Semiconductors > 2022 > 43(3): 032001

Kunal B. Modi, Pooja Y. Raval, Dolly J. Parekh, Shrey K. Modi, Niketa P. Joshi, Akshay R. Makadiya, Nimish H. Vasoya, Utpal S. Joshi. Fe3+-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu3Ti4O12[J]. Journal of Semiconductors, 2022, 43(3): 032001. doi: 10.1088/1674-4926/43/3/032001 ****K B Modi, P Y Raval, D J Parekh, S K Modi, N P Joshi, A R Makadiya, N H Vasoya, U S Joshi, Fe3+-substitution effect on the thermal variation of J–E characteristics and DC resistivity of quadruple perovskite CaCu3Ti4O12[J]. J. Semicond., 2022, 43(3): 032001. doi: 10.1088/1674-4926/43/3/032001.

Citation:

PDF( 1868 KB)