Tailoring the Structure, Energy Storage, Strain, and Dielectric Properties of Bi0.5(Na0.82K0.18)0.5TiO3 Ceramics by (Fe1/4Sc1/4Nb1/2)4+ Multiple Complex Ions

The effects of (Fe_1/4Sc_1/4Nb_1/2)⁴⁺ (FSN) multiple complex ions on the structure and electrical properties of Bi_0.5(Na_0.82K_0.18)_0.5Ti_(1−x)(Fe_1/4Sc_1/4Nb_1/2)_xO₃ (BNKT-xFSN) ceramics were studied. The FSN complex ions induce the phase transition from ferroelectric state to relaxor state. The coercive field and remanent polarization decrease rapidly with the increase of FSN content. With the increase of the external electric field, the energy storage density of BNKT-xFSN ceramics gradually increases and reaches the maximum value of 0.96 J/cm³ (90 kV/cm) at x = 0.09, and the corresponding efficiency is 62%. Meanwhile, the field-induced strain of BNKT-0.07FSN ceramic increases from 0.13% at 50 kV/cm to 0.43% at 80 kV/cm, and the corresponding electrostrictive coefficient Q₃₃ reaches the maximum value of 0.0213 m⁴/C². BNKT-xFSN relaxed ceramics with pseudo-cubic structure have large electrostrictive coefficients when T_d is near room temperature. The local composition inhomogeneity by FSN complex ions at B-sites induces the relaxor characteristics of BNKT-xFSN ceramics.

Introduction

Lead-free ceramics with ABO₃ perovskite structure are very important part of dielectric materials. Ceramics with perovskite structure are often used in the fields of electronic information, aerospace, defense, and military, and have broad application prospects in the future. It is generally known that pure Bi_0.5Na_0.5TiO₃ (BNT) ceramics are difficult to be practical. However, the modified BNT based ceramics have excellent ferroelectric, piezoelectric and dielectric properties and so on, and are considered to be one of the potential materials to replace lead-based ceramics. By introducing the second phase into the BNT matrix, such as BaTiO₃ (BT), Na_0.5Bi_0.5TiO₃ (BKT), the as-formed solid-solution with morphotropic phase boundary (MPB) can be constructed to optimize the structure and properties of BNT-based ceramics (Chen, 2006; Yang et al., 2008; Machado et al., 2016). For example, BNT-BKT solid solution with phases in the vicinity of MPB exhibits excellent electrical properties, such as ferroelectric, dielectric, piezoelectric, strain, and energy storage (Chandrasekhar and Kumar, 2015; Cheng et al., 2015; Li et al., 2015; Guerra et al., 2017; Hajra et al., 2018).

Ion doping as well as solid solution method with ABO₃-type perovskite components (Zou et al., 2010; Zheng and Zuo, 2017; Sui et al., 2019; Zhao et al., 2019) is another common way to modify BNT-based ceramics. Single ion doping substitution is an effective method, such as La³⁺, Ta⁵⁺ ions. There are a few works on complex ions doped BNT-based ceramics. However, complex ions doped BNT-based ceramics illustrate excellent electrical properties, such as energy storage, piezoelectric, strain. Zhao et al. obtained a high energy storage density of 1.41 J/cm³ for BNKT ceramics by the B-site doping of (Al_0.5Nb_0.5)⁴⁺ complex ions (Zhao et al., 2016). The (Al_0.5Nb_0.5)⁴⁺ complex ions doped BNT-BT ceramics illustrated high piezoelectric constant of 210 pC/N and large strain response of 0.29% (Hang et al., 2018). Xie et al. doped (Mg_1/3Nb_2/3)⁴⁺ complex ion into BNKT ceramics, which results in phase change from the ferroelectric phase to ergodic relaxor ferroelectric phase (Xie et al., 2018).

Smolensky et al. first synthesized PMN ferroelectric material with A(B′_1/3B″_2/3)O₃ composite perovskite structure (Smolensky et al., 1976). The A(B′_1/3B″_2/3)O₃ structure also can be equivalently written as A[(B′_2/3B″_1/3)_1/2B″_1/2]O₃. Therefore, the B-sites of A[(B′_2/3B″_1/3)_1/2B″_1/2]O₃ structure have complex ions, which may illustrates some interesting phenomenon. However, as all we known, these multiple complex ions used for lead-free ceramics has not been reported. Based on the adjustability of structure and properties originating from complex ions, multiple complex ions constructed by three elements are used to modify the B-sites of BNT based ceramics. The B-sites of BNT based ceramics are randomly occupied by as-designed multiple complex ions. The chemical composition inhomogeneity originating from the disorder of ions results in the phase transition and improvement of the electrical properties.

The (Sc_1/2Nb_1/2)⁴⁺ complex ions were used to modify the phase structure, growth, dielectric and ferroelectric properties of Pb(Sc_1/2Nb_1/2)_1−xTi_xO₃ single crystals and ceramics, and (1–x)Ba(Sc_1/2Nb_1/2)O₃-xPbTiO₃ solid solution (Bing and Ye, 2003; Wei et al., 2009; Tennery et al., 2010). BNT-BKT solid solution doped with (Fe_1/2Nb_1/2)⁴⁺ complex ions shows high field strain and excellent piezoelectric properties (Fan et al., 2018). Therefore, the Fe³⁺, Sc³⁺, and Nb⁵⁺ ions are selected to construct (Fe_1/4Sc_1/4Nb_1/2)⁴⁺ (FSN) multiple complex ions, which can be equivalently written as [(Fe_1/2Nb_1/2)_1/2(Sc_1/2Nb_1/2)_1/2]⁴⁺. The FSN complex ions were used to modify the phase transition, ferroelectric, energy storage, strain, and relaxation properties of BNT-BKT ceramics.

Experimental Procedure

The Bi_0.5(Na_0.82K_0.18)_0.5Ti_1−x(Fe_1/4Sc_1/4Nb_1/2)_xO₃ (BNKT-xFSN) ceramics with different FNS complex ions contents (x = 0, 0.03, 0.05, 0.07, 0.09, 0.10) were prepared by the solid-state reaction sintering technique. The raw materials of BNKT-xFSN ceramics included high purity oxide powders (Bi₂O₃, Sc₂O₃, Nb₂O₅, Fe₂O₃, TiO₂) and carbonate (K₂CO₃, Na₂CO₃). All of the raw powders were dried at 90°C for at least 1 day, and then weighed according to the stoichiometric formula. The weighed raw powders are mechanically milled by ethanol and zirconium balls for 12 h and then dried at 90°C. The mixed powders were calcinated at 850°C for 2 h to obtain BNKT-xFSN powders. The BNKT-xFSN powders were granulated and added 0.8% polyvinyl alcohol (PVA) as the binder. The 0.35 g granulated powders were pressed at 40 MPa to prepare green body with a diameter of 13 mm. After removing the PVA binder at 600°C for 2 h, The BNKT-xFSN ceramics were sintered at 1,130°C for 2 h. The sintered samples were polished to a thickness of 0.32–0.42 mm. The polished samples were coated with silver electrodes on both sides and fired at 600°C for 0.5 h.

The phase structure of BNKT-xFSN ceramics was analyzed by X-ray diffraction (XRD, D8-Advance, Bruker). The surface morphology of BNKT-xFSN ceramics was analyzed by field emission scanning electron microscopy (FESEM, Quanta 450FEG, FEI). The dielectric properties of BNKT-xFSN ceramics were measured using an impedance analyzer (4294A, Agilent) and a computer-controlled electrical furnace. Ferroelectricity and strain properties were measured by ferroelectric test system (P-PMF, Radiant).

Results and Discussion

Figure 1A presents the XRD diffraction patterns of BNKT-xFSN ceramics. It can be seen that BNKT-xFSN ceramics show pure perovskite structure with no impurity phases. The FSN complex ions are completely dissolved in the BNKT solid solution and also form a new solid solution. An enlarged view of the (200) peaks in the range of 45~48° is shown in Figure 1B. The (200) peak has no splitting peak, which means that BNKT-xFSN ceramic is a pseudo-cubic phase structure. In addition, the (200) peaks shift to the lower angle with increasing FSN complex ions, which is due to the FNS complex ions with larger average ionic radius (Fe³⁺: 0.645 Å; Sc³⁺: 0.745 Å; Nb⁵⁺: 0.640 Å) substituting for Ti⁴⁺ (0.605 Å) ions. This results in the expansion of lattice of BNKT matrix, which is confirmed by the shifting of the (200) diffraction peaks.

FIGURE 1

Figure 1. (A) XRD patterns of BNKT-xFSN ceramics, (B) the magnified view of the (200) peaks.

Figure 2 shows the surface topography and particle size distribution of BNKT-xFSN ceramics. We can see that the structure of BNKT-xFSN ceramics is dense and has no pores, and the grain boundaries are clear. It can be seen from the particle size distribution that the average grain size of BNKT-xFSN ceramic decreases from 5.91 μm at x = 0.01 to 3.04 μm at x = 0.09. When the FNS complex ions content is further increased to 0.10, the average grain size hardly increases. Therefore, the FNS complex ions can refine the grains of BNKT ceramics, the average grain size is <6 μm. However, FSN complex ions have no effect on the surface morphology of BNKT-xFSN ceramics.

FIGURE 2

Figure 2. Surface morphology and grain size distribution of BNKT-xFSN ceramics with different FSN contents: (a) 0.01, (b) 0.03, (c) 0.05, (d) 0.07, (e) 0.09, (f) 0.10.

Figure 3 illustrates the P-E hysteresis loops of BNKT-xFSN ceramics under different electric fields. When x < 0.07, it can be seen that the P-E loops are saturated with largely saturated polarization (P_max), remnant polarization (P_r) and coercive field (E_c), indicating the typical ferroelectric behavior. At the composition critical point of x = 0.07, the pinched P-E hysteresis loops can be obtained, which is similar to double hysteresis loops of anti-ferroelectric. The pinched P-E loops gradually decrease the values of P_r and E_c. Further increasing FSN content, the E_c and P_r values almost keep a constant. Therefore, the long-range ordered structure of BNKT-xFSN ceramics is destroyed, and the ferroelectric state changes to the relaxor state. This is attributed to the local disturbance of B-sites by (Fe_1/4Sc_1/4Nb_1/2)⁴⁺ complex ions substituting for Ti⁴⁺ ions. Simultaneously, P_max also shows a slight decrease. It is well-known that an excellent energy storage property should have low P_r, high P_max, large breakdown strength and double hysteresis loops (Qi and Zuo, 2019). When x ≥ 0.07, the P_max increases almost linearly with the increase of the electric field, while the P_r value hardly changes. At relaxor state with pinched loops, the external electric field promotes the increase of the difference between P_max and P_r, which is beneficial to the improvement of energy storage density.

FIGURE 3

Figure 3. P-E loops of BNKT-xFSN ceramics under different external electric fields with different FSN contents: (A) 0.01, (B) 0.03, (C) 0.05, (D) 0.07, (E) 0.09, (F) 0.10.

Figure 4 shows the energy storage density and efficiency of BNKT-xFSN ceramics under different electric fields. When the FSN content is low, the increase of the electric field has little effect on the energy storage density. When x ≥ 0.07, the energy storage density increases linearly with the increase of the external electric field. The storage energy density increases from 0.06 J/cm³ at x = 0.01 (50 kV/cm) to 0.96 J/cm³ at x = 0.09 (90 kV/cm). However, the effect of the external electric field on the energy storage efficiency is not obvious. In particular, the high energy storage efficiency is also obtained at x = 0.09, which is maintained at about 62%.

FIGURE 4

Figure 4. Energy storage (A) density and (B) Efficiency of BNKT-xFSN ceramics under different electric fields.

Figure 5A shows the I-E loops of BNKT-xFSN ceramic measured at 70 kV/cm. It can be seen that two current peaks caused by ferroelectric domain switching near E_c illustrate high current intensity when x = 0.01 and 0.03. However, there are four current peaks observed from the current curves at x ≥ 0.05, which indicates that there are two types of polarization switching under the stimulation of the external electric field. The I₂ current peaks represent the ferroelectric-type (E_c1 < E_c) for the long-range ordered domains being destroyed and forming nanodomains under the external electric field (Guo et al., 2014). This relaxor state gets back to the unstable ferroelectric type with electric field revoked. The I₁ current peaks correspond to the transition process of relaxor-ferroelectric (E_c2 > E_c), which accompanies with the formation and growth of nanodomains (Jing et al., 2017). The obvious four current peaks at x = 0.05 suggest the coexisting of relaxor and the ferroelectric phase (non-ergodic relaxor phase), which is consistent with the results of (Sr_1/3Nb_2/3)⁴⁺ complex ions doped 0.82Bi_0.5Na_0.5TiO₃-0.18Bi_0.5K_0.5TiO₃ ceramics (Zhou et al., 2018). For x ≥ 0.05, the I₁ and I₂ current peaks shift in opposite directions. The I₁ current peak shift to the high field direction and weakens gradually. However, the I₂ current peaks shift to the zero-electric field, indicating that the induced long-range ferroelectric order will return to relaxor state after removing external electric field (Xing et al., 2016). Ma et al. (2012) proposed by transmission electron microscopy that the four current peaks correspond to the transition between the electric field-induced weakly polarized phase (P4bm) and the strongly polarized phase (R3c + P4bm). In particular, as the doping content increases, the I₂ current peaks gradually shifts to the left and appears in the direction of the reverse electric field. Meanwhile, the current intensity gradually weakens, which indicates that the relaxor behavior is gradually enhanced.

FIGURE 5

Figure 5. (A) I-E loops, (B) Bipolar strain loops and (C) Positive strain (S_pos) and negative strain (S_neg) of BNKT-xFSN ceramics at 70kV/cm.

Figure 5B illustrates the bipolar strain loops of BNKT-xFSN ceramics at 70 kV/cm. The positive strain (S_pos) and negative strain (S_neg) under different FSN contents are shown in Figure 5C. It can be seen that the bipolar strain curves of BNKT-xFSN ceramic at x < 0.07 is butterfly-shaped, which corresponds to typical ferroelectricity. With the increase of FSN content, the S_neg decreases and tends to zero because the relaxor of BNKT-xFSN ceramics is enhanced. Moreover, the shape of strain curves changes from butterfly shape to sprout shape. At x = 0.07, the S_pos reaches the maximum value of 0.35%. BNKT-xFSN ceramics also have a large negative strain at x = 0.05, which indicates that the BNKT-xFSN ceramic at x = 0.05 has strong ferroelectricity, and the transition from the ferroelectric state to relaxor state is in a transitional state. When x = 0.07, the negative strain disappears, indicating that the ergodic relaxor phase is the dominated phase, and the field-induced strain reaches the maximum value. When FSN content is further increased, the phase transition is more complete, at which the relaxor state is more stable. Therefore, a larger electric field is required to induce the relaxor-ferroelectric phase transition (Bai et al., 2016).

Figure 6A shows the bipolar strain of BNKT-0.07FSN ceramic under different electric fields. It can be seen that the sprout-shaped strain curves gradually become saturated as the electric field increases, and the value of the positive strain increases almost linearly. When the electric field is >60 kV/cm, the positive strain value increases sharply, this further indicates that a larger electric field is required to trigger the relaxor-ferroelectric phase transition. In addition, the field-induced strain has undergone two different stages. For the first stage, BNKT-0.07FSN ceramic remains ergodic relaxor at low field, and the strain mainly comes from the contribution to electrostriction. In the second phase, when the electric field is increased to a certain extent, the strain suddenly increases due to the transition from the ergodic relaxor state to the ferroelectric state. The maximum strain and dynamic piezoelectric constant (d₃₃^*) are shown in Figure 6B. It can be seen that the maximum positive strain of 0.43% is obtained when the external electric field is increased to 80 kV/cm. The behavior of the corresponding d₃₃^* is similar to strain, and the maximum value of 534 pm/V is obtained at 80 kV/cm. In general, piezoelectric effects, electrostriction, and domain wall motion are used to analyze the contribution to field-induced strain behavior. The degree of hysteresis for BNKT-0.07FSN ceramic has a larger value of 53.5%. High electrostrictive strains with low hysteresis for BNT-based ceramics play an important role in precision instrumentation (Bai et al., 2016).

FIGURE 6

Figure 6. (A) Bipolar strain loops, (B) Maximum strain and d₃₃^* and (C) S-P² loops of BNKT-0.07FSN ceramic under different electric fields and the inset shows Q₃₃ as the function of different external electric fields.

Figure 6C depicts the strain and polarization squared curves of BNKT-0.07FSN ceramics under different electric fields. The electrostrictive coefficient Q₃₃ can be obtained by linear fitting of the S-P² curve. Analyzed from Figure 6C, the S-P² curves exhibit a strong linear relationship. As shown in the inset of Figure 6C, the electric field has little effect on Q₃₃ value, which is similar to the result of BNT-BKT-NN ceramics under different electric fields and temperatures (Bai et al., 2017). At 70 kV/cm, Q₃₃ reaches the maximum value of 0.0213 m⁴/C². Zhang et al. (2010) proposed that the key issue of obtaining high electrostrictive performance for BNT-based relaxor ferroelectric is obtaining pseudocubic phase at room temperature and the depolarization temperature near room temperature or below by adjusting composition. XRD patterns in Figure 1 indicates that BNKT-0.07FSN composition has a pseudocubic structure at room temperature. Simultaneously, the temperature-dependent dielectric spectra as shown in show Figures 7A,E confirm that the depolarization temperature (T_d) of BNKT-xFSN ceramics decreases to room temperature or below. These characteristics meet the above demands, which can explain why BNKT-0.07FSN ceramic has large electrostrictive strain.

FIGURE 7

Figure 7. Temperature-dependent dielectric spectra of polarized BNKT-xFSN ceramics with different FSN contents: (A) 0, (B) 0.01, (C) 0.03, (D) 0.05, (E) 0.07, (F) 0.09, (G) 0.10.

Figure 7 shows the temperature-dependent dielectric spectra of the poled BNKT-xFSN ceramics measured from 10 to 1,000 kHz. It can be seen that there are three dielectric anomalies peaks at T_d, T_p, and T_m, as marked in the figures_. It can be seen from Figure 7B that the first dielectric anomaly peak is located approximately at depolarization temperature T_d (~140°C), which is corresponding to the temperature of the first tanδ peak. It also can be seen from Figure 7 that T_d decreases below room temperature after x ≥ 0.07. Some interesting phenomena are observed in BNT-based ceramics at T_d, such as pinched P-E loops, large electric field-induced strain (Zhang et al., 2007; Guo et al., 2011; Xie et al., 2019). The second dielectric anomaly peak occurs at T_p, which is dependent on the measurement frequency. This phenomenon is named as frequency dispersion, which nearly disappears when the frequency increases to 1 MHz. The last dielectric anomaly peak shows at temperature T_m, at which maximal dielectric constant is achieved. The T_m almost keeps constant at around 280°C and the maximum dielectric constant decreases from 6,685 to 3,531 with increasing doping content. We can observe from Figure 7 that the dielectric peaks at T_m for the samples at x = 0.07–0.10 are relatively broad. Jo et al. (2011) proposed the temperature-dependent dielectric behavior of BNT-based ceramics is attributed to the thermal evolution of ferroelectric polar nanoregions of R3c and weakly polar P4bm symmetry. The broadened T_m peaks and dispersed T_p peaks indicate that BNKT-xFSN ceramics have relaxor behavior. Na⁺, K⁺, Bi³⁺ occupies A-sites in BNT-based ceramics, and Fe³⁺, Ti⁴⁺, Sc³⁺, Nb⁵⁺ occupies B-sites. The difference of ion radius and charge amount form the local field and local elastic field. The local and elastic fields produce PNRs by hindering the long-range ordered dipole moments (Liu et al., 2016). The PNRs leads to the formation of pseudo-cubic structure, which is consistent with the XRD results. The random distribution of A and B-sites cations leads to structural inhomogeneities, which leads to the broadening and dispersion characteristics of the temperature-dependent dielectric spectra.

Based on the above analysis of structure, ferroelectric, strain and dielectric properties, the composition-temperature phase transition of BNKT-xFSN ceramics is summarized as shown in Figure 8. It can be seen that T_d drops almost linearly below room temperature, but the T_m maintains almost a constant. At the same time, it can be inferred that the composition between 0.05 and 0.07 is a critical point in which two phases (ferroelectric phase and ergodic relaxor phase) coexist in the BNKT-xFSN ceramics featured by the shifting of T_d to the room temperature. Due to the reduction of energy barriers, the critical component is usually located in a region where polarization reversal and polarization extension mechanisms are strong (Shi et al., 2014). For x < 0.05, the ferroelectric phase dominates the phase structure. When x ≥ 0.05, the ergodic relaxor phase plays a major role. Therefore, the external stimulation, such as doping, temperature, and electric field, can modify the phase transition between the ferroelectric and relaxor states of BNKT-xFSN ceramics.

FIGURE 8

Figure 8. Temperature-composition phase transition diagram of BNKT-xFSN ceramics.

Conclusion

The phase, microstructural and electrical properties of Bi_0.5(Na_0.82K_0.18)_0.5TiO₃ ceramics were tailored by (Fe_1/4Sc_1/4Nb_1/2)⁴⁺ multiple complex ions. FSN complex ions doped BNKT ceramics illustrate the pseudo-cubic phase and the expansion of lattice. The grains with uniform size are densely packed together. The surface morphology of grains is independent of FSN content, but grain size decreases gradually. FSN doping induces the phase transition from the ferroelectric state to the relaxor state, which illustrates the decrease of P_r and E_c, and the improvement of energy storage and strain. The maximum energy storage density of 0.96 J/cm³ is obtained at x = 0.09 and 90 kV/cm, and the corresponding efficiency is 62%. In addition, the strain of BNKT-0.07FSN ceramics increased from 0.13% at 50 kV/cm to 0.43% at 80 kV/cm, and its electrostrictive coefficient reaches the maximum value of 0.0213 m⁴/C² at 70 kV/cm. The depolarization temperature adjusted by FSN complex ions decrease from 144°C to below room temperature. The B-sites inhomogeneity of BNKT-xFSN ceramics induced by FSN multiple complex ions results in the formation of the relaxor characteristics.

Data Availability Statement

All datasets generated for this study are included in the article/supplementary material.

Author Contributions

ZH and HX conceived and designed the study. ZH, HX, and WQ performed the experiments. ZH, HW, and JX wrote the paper. LY, XZ, CZ, LY, JX, and HW reviewed and edited the manuscript. All authors read and approved the manuscript.

Funding

This work was supported by the National Nature Science Foundation of China (11664006, 61741105, and 61965007). Guangxi Nature Science Foundation (2017GXNSFDA198024 and 2018GXNSFDA281042). Guangxi Key Laboratory of Information Materials (171009-Z) and Innovation Project of GUET Graduate Education (2018YJCX81).

Conflict of Interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

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