Next Article in Journal
Designing of the Electromechanical Drive for Automated Hot Plate Welder Using Load Optimization with Genetic Algorithm
Next Article in Special Issue
Memristive Characteristics of the Single-Layer P-Type CuAlO2 and N-Type ZnO Memristors
Previous Article in Journal
Sustainable Use of Apple Pomace (AP) in Different Industrial Sectors
Previous Article in Special Issue
Seeing Structural Mechanisms of Optimized Piezoelectric and Thermoelectric Bulk Materials through Structural Defect Engineering
 
 
Search for Articles:
Title / Keyword
Author / Affiliation / Email
Journal
Article Type
 
 
Advanced Search
 
Section
Special Issue
Volume
Issue
Number
Page
 
Journals
Materials
Volume 15
Issue 5
10.3390/ma15051789
materials-logo
Submit to this Journal Review for this Journal Propose a Special Issue
► Article Menu

Article Menu

share Share announcement Help format_quote Cite question_answer Discuss in SciProfiles thumb_up
...
Endorse textsms
...
Comment
first_page
settings
Order Article Reprints
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Structure and Electrical Properties of Microwave Sintered BTS-BCT-xBF Lead-Free Piezoelectric Ceramics

by
Tao Wang
1,
Jian Ma
2,
Bo Wu
2,*,
Fenghua Wang
1,
Shiyu Wang
1,
Min Chen
1 and
Wenjuan Wu
1,*
1
Sichuan Province Key Laboratory of Information Materials and Devices Application, Chengdu University of Information Technology, Chengdu 610225, China
2
Sichuan Province Key Laboratory of Information Materials, Southwest Minzu University, Chengdu 610041, China
*
Authors to whom correspondence should be addressed.
Materials 2022, 15(5), 1789; https://doi.org/10.3390/ma15051789
Submission received: 28 December 2021 / Revised: 20 February 2022 / Accepted: 21 February 2022 / Published: 27 February 2022
(This article belongs to the Special Issue Electronic Functional Materials: Synthesis, Structure, Property, Mechanism and Application)
Browse Figures
Versions Notes

Abstract

:
Barium titanate (BT)-based ceramics are one of the promising piezoelectric materials for environment-friendly electro-mechanical transformation. However, high performance materials are often sintered at high temperatures, resulting in volatile components and increased energy consumption. Here, 0.82Ba(Ti0.89Sn0.11)O3-(0.18-x)(Ba0.7Ca0.3)TiO3-xBiFeO3 (BTS-BCT-xBF) piezoelectric ceramics were prepared by microwave sintering (MWS) method, and the structure and properties were emphatically studied, aiming to reveal the regulatory mechanism of MWS on the structure and properties. Compared with conventional solid sintering (CS), the phase structure presents a similar evolution in MWS ceramics as a function of BF, while the more refined grain size and the denser structure are observed in MWS ceramics. The electrical properties (e.g., d33, εr, tan δ, etc.) of MWS ceramics are superior to the CS ceramics owing to the refined grain size and denser microstructure. It is worth noting that the energy storage performance (e.g., energy storage density, energy storage efficiency) significantly outperformed expectations due to the slender hysteresis loop resulting from the smaller grain and high cubic phase. Therefore, the MWS sintering mechanism can further drive practical application of BT-based ceramics.

1. Introduction

As the representative of piezoelectric material, barium titanate (BT)-based ceramics are widely used in electronic components due to their excellent electric properties, such as micro-capacitors, ferroelectric memory, etc. [1,2]. However, the disadvantages, including high sintering temperature, poor temperature stability, and low breakdown field strength, seriously hinder the application in complex environment. In order to further seize the market, many means are used to overcome the shortages of BT-based materials, especially the various ways of preparation [3,4,5].
It is reported that the preparation of piezoelectric ceramics has many options in terms of sintering processes, such as spark plasma sintering (SPS) [6], atmosphere sintering [7], hot pressed sintering [8], microwave sintering (MWS) [9,10], etc. Among those options for sintering, MWS possesses the unique advantage of rapid sintering for materials at low temperature during the preparation process, which have been widely used to synthesize new materials [11,12]. It can also enhance the density of materials significantly, and improve the electrical properties. Takahashi H et al. reported a densified BT-based material system with high d33 prepared by MWS [13]. Bafandeh et al. prepared KNN-based ceramics by conventionally sintering and microwave-sintering, and systematically compared the microstructure, ferroelectric, and piezoelectric properties of those samples, showing that MWS can inhibit grain growth and enhance densification in this ceramic, which results in improvements in the electric properties (e.g., piezoelectric properties, ferroelectric properties, strain behavior, etc.) [14]. The effects of different sintering methods on the phase boundary and microstructure of BT-based ceramics were studied by Gao et al. [15]. Compared with conventional solid sintering (CS), the phase structure of microwave sintering ceramics remains almost stable, and the samples present a smaller grain size and uniform grain distribution. Another advantage of MWS is that it can significantly reduce temperature and time during the sintering process. However, the effects of MWS on the structure and properties have not been investigated sufficiently in BT-based ceramics with high performance. Revealing the regulatory mechanism of MWS on the structure and properties of BT-based ceramics is an urgent aim, which can further enrich strategies for tuning their performance.
Recently, a series of BT-based ceramics with excellent performance have been obtained by constructing multiphase boundaries though chemical modification (e.g., Ca, Sr, Zr, Sn, Hf, etc.). For example, Wang et al. [16] reported (Ba0.85Ca0.15)(Ti0.9Zr0.1)O3 (BCTZ) ceramics with large d33 (~650 pC/N), and Zhu et al. observed a high d33 in (Ba, Ca)TiO3–0.45Ba(Sn,Ti)O3 ceramics. In particular, Zhao et al. reported high piezoelectric properties (d33 = 700 ± 30 pC/N) in 0.82Ba(Ti0.89Sn0.11)O3-0.18(Ba0.7Ca0.3)TiO3 materials, which are comparable to that of lead-based and lead-free based piezoelectric materials. However, the ceramics with optimal piezoelectric properties were always sintered at a relatively high temperature, which could lead to the compositional volatile and increased the energy consumption during the sintering process. Therefore, it is expected that a lower temperature sintering could be used for fabrication, which will cut down the processing costs especially in production.
To further reveal the mechanism of MWS on the structure and properties BT-based ceramics with high performance, the Ba(Ti0.89Sn0.11)O3-(Ba0.7Ca0.3)TiO3 material system was chosen to verify the efficiency of this strategy in BT-based ceramics. In addition, BiFeO3 (BF), a typical ferroelectric material with large Pr and high Tc, was also introduced to this material system, not only aiming to reduce the sintering temperature but also further modify the structure and properties [17,18,19]. For better comparison the effects of MWS and CS on the structure and properties, two sets of 0.82Ba(Ti0.89Sn0.11)O3-(0.18-x)(Ba0.7Ca0.3)TiO3-xBiFeO3 (BTS-BCT-xBF) samples were prepared by MWS and CS, aiming to reveal the regulatory mechanism of MWS and CS on the structure and electrical properties of lead-free piezoelectric ceramics, which may promote the practical application of BT-based ceramics.

2. Experimental Procedure

The 0.82Ba(Ti0.89Sn0.11)O3-(0.18-x)(Ba0.7Ca0.3)TiO3-xBiFeO3(BTS-BCT-xBF, x = 0.002, 0.004, 0.006, 0.008, 0.010, 0.012) piezoelectric ceramics were prepared by microwave sintering and normal sintering. Raw materials, including BaCO3 (99.0%), CaCO3 (99.0%), SnO2 (99.5%), TiO2 (98%), Bi2O3, and Fe2O3 (99%), were mixed with ZrO2 balls and the medium of ethanol for 12 h in planetary ball mill. After being dried in oven and calcined at 1200 °C for 2 h, these powders were mixed with polyvinyl alcohol (PVA, 7–8 wt%) and pressed into pellets of ~10 mm in diameter and ~1 mm in thickness. After the PVA binder burned out, the pellets were divided into two groups. One group was sintered at 1350 °C for 3 h by conventional sintering method, and the other group was sintered at 1290 °C for 2 h by microwave sintering method. Silver paste was used as electrodes for electrical measurements, and was fired at ~650 °C for 30 min. These samples were poled in a silicone oil bath under a dc field of ~3.0 kV/mm for 30 min.
X-ray diffractometer (XRD) with a CuKα radiation (DX-2700, Haoyuan Instrument, Dandong, China) was used to confirm phase structure of the samples under ~40 kV, ~30 mA. Their microstructure and chemical compositions were measured by a field-emission scanning electron microscope (FE-SEM) (JSM-7500, JEOL, Showa, Japan). The dielectric constant (εr) varying with temperature (−150–200 °C) was measured by using an LCR analyzer (HP 4980, Agilent, Palo Alto, USA) in connection with a temperature-controlled instrument. The polarization versus electric field (P-E) hysteresis loops and the strain-electric field (S–E) curves were measured at 1 Hz with a ferroelectric tester (Radiant Premier II, Radiant Technologies, Inc., Albuquerque, NM, USA). The d33 value was measured by a d33 m (ZJ-3A, Zhichuang Technology Development Co., Ltd., Beijing, China) for the poled samples.

3. Results and Discussion

3.1. Phase Structure

Figure 1a,b plots room temperature XRD patterns of BTS-BCT-xBF ceramics in the 2θ range of ~20–60° sintered with MWS and CS, respectively. Compared with the standard cards’ diffraction peaks of R (PDF # 85-1797), O (PDF # 81-2200), and T (PDF # 05-0626) in BaTiO3 materials, all ceramics show a pure perovskite structure without any other phase, indicating that BTS-BCT and BF formed multiphase ceramics within the study range of 0.002 ≤ x ≤0.012. In addition, the effect of BF content on the phase structure of BTS-BCT-xBF ceramics sintered with different sintering methods was analyzed by the enlarged XRD pattern with multi-peak fitting via Lorentz method (see Figure 1c,f) [20,21]. There are four separated peaks ((002)T, (200)T, (022)O and (200)O) in the XRD pattern of the ceramics with x = 0.002, and three characteristics peaks ((020)R, (002)T and (200)T) in the ceramics with x = 0.004, indicating that the sintering method did not change the phase structure of the ceramics.
Figure 2 shows the εr-T curves (−80–120 °C) of BTS-BCT-xBF ceramics prepared by MWS and CS, measured at 1~100 kHz, which aimed to further verify the phase structure of BTS-BCT-xBF ceramics sintered with MWS and CS. Three dielectric peaks are observed in the curve of the ceramics with x = 0.002, corresponding to the rhombohedral-orthorhombic (R-O) phase transition temperature (TR-O) at lower temperature, the orthorhombic-tetragonal (O-T) phase transition temperature (TO-T) near room temperature, and the Curie temperature (Tc) at high temperature, respectively. Only two dielectric peaks are observed in the curves of the ceramics with x > 0.002, which is related to the rhombohedral-tetragonal (R-T) phase transition temperature (TR-T) at lower temperature and Curie temperature (Tc) at high temperature, respectively. One can see that the phase boundaries are very sensitive to BF content, as shown in Figure 2a–f. Compared with CS samples of x = 0.002, the TO-T (MWS: ~25 °C, CS: ~28 °C) and TR-O (MWS: ~6 °C, CS: ~10 °C) moves towards low temperature, and the Tc (MWS: ~52 °C, CS: ~53 °C) keeps almost stable in MWS ceramics, indicating that the O-T phase boundaries is obtained near room temperature. With increasing BF to 0.004, all ceramics show R-T phase boundaries because the O-T and R-O phases form a convergence zone near room temperature, and the TR-T of MWS sample is higher than the CS ceramics. With further increasing BF, the TR-T and Tc decrease simultaneously, and the T-C phase boundaries are observed near room temperature in those ceramics. In addition, Tc of MWS ceramics (52 °C→22 °C) changes faster than CS ceramics (53 °C→39 °C) in BTS-BCT-xBF ceramics. Figure 2g,h plots the phase diagram of MWS and CS BTS-BCT-xBF ceramics. The evolution of phase boundaries is highly matched with the XRD patterns, that is, O-T for 0.002 ≤ x < 0.004, R-T for 0.004 ≤ x < 0.006, and T-C for x ≥ 0.006.
Figure 3 plots the modified Curie-Weiss law (ln(1/εr − 1/εm) − ln(T −Tm)) of BST-BCT-xBF ceramic, which is originated from the following formula:
1/εr − 1/εm = (T − Tm)γ/C,
where εm is the maximum value of relative dielectric constant and γ is the degree of diffuseness. The higher γ value is observed in MWS ceramics, indicating that the MWS ceramics show a stronger relaxation degree than the CS ceramics. This can be ascribed to the smaller grain sizes in MWS ceramics, which will be discussed later.

3.2. Microstructure

Figure 4a–d and Figure S1 (see the Supplementary Materials) show the SEM surface morphology of MWS ceramics. A phenomenon of bimodal distribution of large and small grains is observed in MWS ceramics with 0.002 ≤ x ≤ 0.004. The average grain size of large grains is about 43.65~47.96 μm, and the small grains of 1.0~1.8 μm surround the large grains, resulting in the improved density by filling the pores around the large grains, and the average grain size decreases from 29.14 μm to 23.60 μm. With further increasing BF in MWS ceramics, the average grain size decreases from 21.25 μm to 13.99 μm, and the bimodal distribution of grain disappears in those ceramics. Figure 4e–h shows the SEM of CS BTS-BCT-BF ceramics. It is found that the grain size tends to be smaller with the increase of BF content, that is, it decreases from 56.72 μm to 18.50 μm as a function of BF, suggesting that the excess BF can inhibit the grain growth. Compared with CS samples, the grain size is smaller in MWS ceramics (see Figure 4i), proving that the MWS method can also hinder the growth of grain in ceramics; such a phenomenon has been obtained elsewhere [22,23,24]. Significantly, the grain size of MWS BTS-BCT-xBF ceramics is close to CS with the increase of doping concentration starting from 0.008, while still a little smaller than the grain size of CS. This can be explained by the synthetic effect of MWS and high concentrations of BF. The effect of MWS has a major role in decreasing grain sizes at x < 0.008, and high concentrations of BF play an important role in decreasing grain sizes at x ≥ 0.008. In addition, the synthetic effect of MWS and high concentrations of BF on the grain sizes lead to a little smaller grain size in MWS than CS at x ≥ 0.008. In addition, the variation of relaxation degree can be ascribed to the evolution of grain size, as shown in Figure 3 and Figure 4. The decrease of grain size results in an increase of the internal stress induced by lattice distortion, which can change the forces between the short-range and long-range, thus the relaxation behavior of MWS ceramics is stronger than the CS. The density of the ceramics is measured through Archimedes drainage method, as shown in Table 1. One can find that the density first increases and then decreases in the samples as a function of BF, and the density of MWS ceramics is higher than CS ceramics, indicating that MWS plays a more effective role in enhancing density.

3.3. Dielectric and Ferroelectric Properties

Figure 5a,b shows the P-E and S-E loops for MWS and CS ceramics, measured at room temperature and 30 kV/cm. All samples present saturated P-E loops and standard S-E curves, indicating that all samples are normal ferroelectrics. Due to the high Pr for BF, the Pr increases with increasing the proper BF, and the ferroelectric properties would deteriorate in the ceramics with adding excessive BF, as shown in Figure 6a. The Pr of MWS samples is smaller than that of CS ceramics, which results from the grain refinement leading to a decrease in Pr due to the increased clamping effect of domain walls relative to grain boundaries [25,26]. Compared with the CS samples with x > 0.004, the Pr decreases sharply in MWS samples, which is related to the evolution of phase boundary. With increasing BF content, the cubic phase of MWS ceramics gradually dominates in the phase structure near room temperature, and then results in deteriorating of the ferroelectric properties. The Ec of two group samples keeps almost unchanged with increasing BF content, as shown in Figure 6b. The Spos (the strain between the maximum strain and the strain under 0 kV/cm) of MWS and CS ceramics are shown in Figure 6c, which first increases and then decreases with increasing BF, achieving maximum Spos value (MWS: ~0.102%, CS: ~0.105%) at the ceramics with x = 0.004, which can be ascribed to the low energy barrier in multiphase boundary. Moreover, the maximum strain in MWS ceramics is lower than CS due to the limitation of a large number of fine grain when x ≤ 0.004. Figure 6d plots the dielectric constant (εr) of CS and MWS ceramics, measured at 10 kHz. The εr increases continuously in MWS ceramics, while first decreasing and then increasing in CS ceramics with increasing BF. The higher εr of MWS ceramics results from the finer grains because εr increases with decreasing grain size when the average grain size is greater than 1.2 µm [27,28]. Of course, the high density of MWS ceramics also contributes positively to this. The dielectric loss (tan δ) of two sets of samples is very close, and remains around 0.02~0.04, as shown in Figure 6e. This suggests that the tan δ is not sensitive to the sintering methods, and this phenomenon has been reported in other BT-based ceramics [29]. The d33 of MWS and CS ceramics presents a similar change trend, as shown in Figure 6f. That is, d33 first increases and then decreases with the increase of BF content, reaching the maximum values (MWS: ~425 pC/N, CS: ~360 pC/N) at x = 0.004. This can be attributed to the R-T phase boundaries near room temperature in the ceramic with x = 0.004. As is known, multiphase coexistence provides more possible polarization directions, resulting in easy polarization rotation, which can greatly facilitate the polarization switching [30]. Moreover, the bimodal grain sizes distribution can also enhance the d33 value in MWS ceramics [25].

3.4. Energy Storage Performance and Electrostriction

Figure 7a shows the P-E loops of the MWS and CS ceramics with x = 0.012. It is reported that the thinner P-E loop with high Pmax and low Pr value is beneficial to energy storage due to the low energy loss in the materials. Compared with the P-E loops of CS ceramics, a thinner P-E loop is obtained in MWS ceramics, indicating that it has better energy storage performance than CS ceramics. To further make a quantitative analysis on the energy storage performance of MWS and CS ceramics, the calculated energy storage performance of MWS and CS ceramics with x = 0.012 are plotted in Figure 7b,c, measured at 30 kV/cm. As is known, the discharge storage density W1 can be obtained from the integration of the discharge curve, and the area between the charge Curve and the discharge curve is the energy loss W2, η = W1/(W1 + W2) is used to express energy storage efficiency [31,32,33]. Although the Pmax of MWS ceramics is slightly lower than that of CS, the MWS ceramics have better energy storage density and energy storage efficiency (MWS: W1 = 0.1019 J/cm3, η = 90.10%; CS: W1 = 0.0883 J/cm3, η = 73.46%) due to the slender hysteresis loop resulting from the smaller grain and high cubic phase. Therefore, MWS may be beneficial to the enhanced energy storage performance. Polarization reveals that the strain is mainly contributed by electrostriction in the ceramics, and the S-P curves of some components deviate from the quadratic relationship caused by the irreversible domain switching [34,35,36,37,38,39]. The Q33 of the ceramics shows a similar trend, that is, Q33 increases first and then decreases, and reaches the maximum value at x = 0.004 (MWS: ~0.049 m4/C2, CS: ~0.045 m4/C2), as shown in Figure 8. Moreover, the MWS ceramics have higher Q33 than CS.

4. Conclusions

In this work, 0.82Ba(Ti0.82Sn0.11)O3-(0.18-x)(Ba0.7Ca0.3)TiO3-xBiFeO3 (BTS-BCT-xBF) piezoelectric ceramics were prepared by microwave sintering method and conventional sintering method. The phase structure of two group samples presents a similar evolution, and the more refined grain size was observed in MWS ceramics, resulting in the denser structure than CS ceramics. Owing to the refined grain size and denser microstructure in MWS ceramics, the electrical properties (e.g., εr~8273, d33~425 pC/N, tan δ~0.022, Strain~0.102%, Q33~0.049 m4/C2) were better than the performance of CS ceramics (e.g., εr~5400, d33~360 pC/N, tan δ~0.026, Strain~0.105%, Q33~0.045 m4/C2). In addition, the energy storage performance (e.g., energy storage density, energy storage efficiency) significantly outperformed expectations due to the slender hysteresis loop resulting from the smaller grain and high cubic phase, and the Q33 in MWS ceramics was also superior to the CS ceramics.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/ma15051789/s1, Figure S1: Surface morphology images of the BTS-BCT-xBF ceramics sintered by (a,b) MWS and (c,d) CS.

Author Contributions

Conceptualization, investigation and methodology—B.W. and W.W.; experimentation and data acquisition—T.W., F.W. and S.W.; analysis and interpretation—J.M.; writing-original draft preparation—T.W. and B.W.; writing-review and editing—M.C. and W.W. All authors have read and agreed to the published version of the manuscript.

Funding

Authors gratefully acknowledge the support of the National Science Foundations of China (NSFC Nos. 51702028, 51702029), the Foundation of Sichuan province science and technology support program (Grant No. 2021YJ0560, 22ZDYF3306), and the Fundamental Research Funds for the Central Universities, Southwest Minzu University (No. 2020NTD03).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data that support the findings of this study are available within this article.

Conflicts of Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

References

  1. Zhao, C.; Wu, H.; Li, F.; Cai, Y.; Zhang, Y.; Song, D.; Wu, J.; Lyu, X.; Yin, J.; Xiao, D.; et al. Practical high piezoelectricity in barium titanate ceramics utilizing multiphase convergence with broad structural flexibility. J. Am. Chem. Soc. 2018, 140, 15252–15260. [Google Scholar] [CrossRef]
  2. Wu, B.; Wu, H.; Wu, J.; Xiao, D.; Zhu, J.; Pennycook, S.J. Giant piezoelectricity and high curie temperature in nanostructured alkali niobate lead-free piezoceramics through phase coexistence. J. Am. Chem. Soc. 2016, 138, 15459–15464. [Google Scholar] [CrossRef]
  3. Gu, H.; Zhu, K.; Pang, X.; Shao, B.; Qiu, J.; Ji, H. Synthesis of (K, Na) (Nb, Ta)O3 lead-free piezoelectric ceramic powders by high temperature mixing method under hydrothermal conditions. Ceram. Int. 2012, 38, 1807–1813. [Google Scholar] [CrossRef]
  4. Krishna, T.; Anuradha, S.; Mamta, S.; Arun, K. Factors affecting morphological and electrical properties of barium titanate: A brief review. Mater. Today 2021, 44, 4548–4556. [Google Scholar]
  5. Bai, Y.; Matousek, A.; Tofel, P.; Bijalwan, V.; Nan, B.; Hughes, H.; Button, T.W. (Ba, Ca)(Zr, Ti)O3 lead-free piezoelectric ceramics—the critical role of processing on properties. J. Eur. Ceram. Soc. 2015, 35, 3445–3456. [Google Scholar] [CrossRef]
  6. Yang, W.; Li, P.; Wu, S.; Li, F.; Shen, B.; Zhai, J. A Study on the relationship between grain size and electrical properties in (K, Na)NbO3-based lead-free piezoelectric ceramics. Adv. Electron. Mater. 2019, 5, 1900570. [Google Scholar] [CrossRef]
  7. Noritake, K.; Sakamoto, W.; Yuitoo, I.; Takeuchi, T.; Hayashi, K.; Yogo, T. Fabrication of lead-free piezoelectric Li2CO3-added (Ba, Ca)(Ti, Sn)O3 ceramics under controlled low oxygen partial pressure and their properties. Jpn. J. Appl. Phys. 2017, 57, 1347–4065. [Google Scholar]
  8. Jean, F.; Schoenstein, F.; Zaghrioui, M.; Bah, M.; Marchet, P.; Bustillo, J.; Giovannelli, F.; Monot-Laffez, I. Composite microstructures and piezoelectric properties in tantalum substituted lead-free K0.5Na0.5Nb1-xTaxO3 ceramics. Ceram. Int. 2018, 44, 9463–9471. [Google Scholar] [CrossRef] [Green Version]
  9. Ji, C.; Fan, T.; Chen, G.; Bai, X.; Wang, J.; He, J.; Cai, W.; Gao, R.; Deng, X.; Wang, Z.; et al. Influence of sintering method on microstructure, electrical and magnetic properties of BiFeO3–BaTiO3 solid solution ceramics. Mater. Today Chem. 2021, 20, 100419. [Google Scholar] [CrossRef]
  10. Cai, E.; Liu, Q.; Zeng, F.; Wang, Y.; Xue, A. A comparative study of lead-free (Ba0.85Ca0.15)(Ti0.9Zr0.08Sn0.02)O3 ceramics prepared by conventional sintering and microwave sintering techniques. Ceram Int. 2018, 44, 788–798. [Google Scholar] [CrossRef]
  11. Guillén, R.M.; Benavente, R.; Salvador, M.D.; Pearanda, F.L.; Borrell, A. Dielectric, mechanical and thermal properties of ZrO2–TiO2 materials obtained by microwave sintering at low temperature. Ceram Int. 2021, 47, 27334–27341. [Google Scholar] [CrossRef]
  12. Mane, S.M.; Pawar, S.A.; Patil, D.S.; Kulkarni, S.B.; Tayade, N.T.; Shin, J.C. Magnetoelectric, magnetodielectric effect and dielectric, magnetic properties of microwave-sintered lead-free x(Co0.9Ni0.1Fe2O4)-(1-x)[0.5(Ba0.7Ca0.3TiO3) -0.5(BaZr0.2Ti0.8O3)] particulate multiferroic composite. Ceram. Int. 2020, 46, 3311–3323. [Google Scholar] [CrossRef]
  13. Takahashi, H.; Numamoto, Y.; Tani, J.; Matsuta, K.; Qiu, J.; Tsurekawa, S. Lead-free barium titanate ceramics with large piezoelectric constant fabricated by microwave sintering. Jpn. J. Appl. Phys. 2006, 45, L30–L32. [Google Scholar] [CrossRef]
  14. Bafandeh, M.R.; Gharahkhani, R.; Abbasi, M.H.; Saidi, A.; Lee, J.S.; Han, H.S. Improvement of piezoelectric and ferroelectric properties in (K, Na)NbO3-based ceramics via microwave sintering. J. Electroceram. 2014, 33, 128–133. [Google Scholar] [CrossRef]
  15. Gao, P.; Pu, Y.; Wu, Y.; Li, P. A comparative study on positive temperature coefficient effect of BaTiO3–K0.5Bi0.5TiO3 ceramics by conventional and microwave sintering. Ceram. Inter. 2014, 40, 637–642. [Google Scholar] [CrossRef]
  16. Wang, P.; Li, Y.; Lu, Y. Enhanced piezoelectric properties of (Ba0.85Ca0.15)(Ti0.9Zr0.1)O3, lead-free ceramics by optimizing calcination and sintering temperature. J. Eur. Ceram. Soc. 2011, 31, 2005–2012. [Google Scholar] [CrossRef]
  17. Wang, D.; Wang, M.; Liu, F.; Cui, Y.; Zhao, Q.; Sun, H.; Jin, H.; Cao, M. Sol–gel synthesis of Nd-doped BiFeO3 multiferroic and its characterization. Ceram. Int. 2015, 41, 8768–8772. [Google Scholar] [CrossRef]
  18. Sun, X.; Chen, J.; Yu, R.; Xing, X.; Qiao, L.; Liu, G. BiFeO3-doped (Na0.5K0.5)NbO3 lead-free piezoelectric ceramics. Sci. Technol. Adv. Mater. 2008, 9, 025004. [Google Scholar] [CrossRef] [Green Version]
  19. Zuo, R.; Ye, C.; Fang, X. Na0.5K0.5NbO3–BiFeO3 lead-free piezoelectric ceramics. J. Phys. Chem. Solids 2008, 69, 230–235. [Google Scholar] [CrossRef]
  20. Bai, Q.; Ma, J.; Wu, W.; Zheng, C.; Wu, B.; Chen, M. Superior electrostrictive coefficient of 6BNT-4SCxBT lead-free relaxor ferroelectrics with Ca2+ substitution. Ceram. Int. 2020, 46, 17691–17697. [Google Scholar] [CrossRef]
  21. Wu, W.; Ma, J.; Wang, N.; Shi, C.; Chen, K.; Zhu, Y.; Chen, M.; Wu, B. Electrical properties, strain stability and electrostrictive behavior in 0.5BaZr0.2Ti0.8O3-(0.5-x)Ba0.7Ca0.3TiO3-xBa0.7Sr0.3TiO3 lead-free ceramics. J. Alloys. Compd. 2019, 814, 152240. [Google Scholar] [CrossRef]
  22. Devi, H.S.; Maisnam, M. Microwave sintering effect on the structural and electrical properties of sodium potassium niobate nanocrystallites. Integr. Ferroelectr. 2019, 202, 204–209. [Google Scholar] [CrossRef]
  23. Swain, S.; Kumar, P.; Agrawal, D.K.; Sonia. Dielectric and ferroelectric study of KNN modified NBT ceramics synthesized by microwave processing technique. Ceram. Int. 2013, 39, 3205–3210. [Google Scholar] [CrossRef]
  24. Kang, J.K.; Dinh, T.H.; Lee, C.H.; Han, H.S.; Tran, V.D.N. Comparative study of conventional and microwave sintering of large strain Bi-based perovskite ceramics. Trans. Electr. Electron. Mater. 2017, 18, 1–6. [Google Scholar] [CrossRef]
  25. Zhao, Z.; Buscaglia, V.; Viviani, M.; Buscaglia, M.T.; Mitoseriu, L.; Testino, A.; Nygren, M.; Johnsson, M.; Nanni, P. Grain-size effects on the ferroelectric behavior of dense nanocrystalline BaTiO3 ceramics. Phys. Rev. B 2004, 70, 024107. [Google Scholar] [CrossRef]
  26. Dupuy, A.D.; Kodera, Y.; Carman, G.P.; Garay, J.E. Effect of phase homogeneity and grain size on ferroelectric properties of 0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Ca0.3) TiO3(BXT) lead-free ceramics. Scr. Mater. 2019, 159, 13–17. [Google Scholar]
  27. Hoshina, T.; Furuta, T.; Yamazaki, T.; Takeda, H.; Tsurumi, T. Grain size effect on dielectric properties of Ba0.92Ca0.08TiO3 ceramics. Jpn. J. Appl. Phys. 2013, 52, 09KC05.1–09KC05.6. [Google Scholar] [CrossRef]
  28. Hoshina, T.; Furuta, T.; Yamazaki, T.; Takeda, H.; Tsurumi, T. Grain size effect on dielectric properties of Ba(Zr, Ti)O3 ceramics. Jpn. J. Appl. Phys. 2012, 51, 09LC04.1–09LC04.5. [Google Scholar] [CrossRef]
  29. Orlik, K.; Lorgouilloux, Y.; Marchet, P.; Thuault, A.; Jean, F.; Rguiti, M.; Courtois, C. Influence of microwave sintering on electrical properties of BCTZ lead free piezoelectric ceramics. J. Eur. Ceram. Soc. 2020, 40, 1212–1216. [Google Scholar] [CrossRef]
  30. Kalyani, A.K.; Brajesh, K.; Senyshyn, A.; Ranjian, R. Orthorhombic-tetragonal phase coexistence and enhanced piezo-response at room temperature in Zr, Sn, and Hf modified BaTiO3. Appl. Phys. Lett. 2014, 104, 252906. [Google Scholar] [CrossRef]
  31. Yuan, Q.; Yao, F.; Wang, Y.; Ma, R.; Wang, H. Relaxor ferroelectric 0.9BaTiO3-0.1Bi(Zn0.5Zr0.5)O3 ceramic capacitors with high energy density and temperature stable energy storage properties. J. Mater. Chem. C 2017, 5, 9552–9558. [Google Scholar] [CrossRef]
  32. Wu, L.; Wang, X.; Li, L. Lead-free BaTiO3-Bi(Zn2/3Nb1/3)O3 weakly coupled relaxor ferroelectric materials for energy storage. RSC. Adv. 2016, 6, 14273–14282. [Google Scholar] [CrossRef]
  33. Wang, G.; Lu, Z.; Li, J.; Ji, H.; Yang, H.; Li, L.; Sun, S.; Feteira, A.; Yang, H.; Zuo, R.; et al. Lead-free (Ba, Sr)TiO3–BiFeO3 based multilayer ceramic capacitors with high energy density. J. Eur. Ceram. Soc. 2020, 40, 1779–1783. [Google Scholar] [CrossRef]
  34. Rauls, M.B.; Dong, W.; Huber, J.E.; Lynch, C.S. The effect of temperature on the large field electromechanical response of relaxor ferroelectric 8/65/35 PLZT. Acta. Mater. 2011, 59, 2713–2722. [Google Scholar] [CrossRef]
  35. Zhu, Y. Large electrostrictive properties in lead free BaTiO3–ZnSnO3 solid solutions. Appl. Phys. A 2019, 125, 301. [Google Scholar] [CrossRef]
  36. Li, F.; Jin, L.; Guo, R. High electrostrictive coefficient Q33 in lead-free Ba(Zr0.2Ti0.8)O3-x(Ba0.7Ca0.3)TiO3 piezoelectric ceramics. Appl. Phys. Lett. 2014, 105, 232903. [Google Scholar] [CrossRef]
  37. Zuo, R.; Qi, H.; Fu, J.; Li, J.; Shi, M.; Xu, Y. Giant electrostrictive effects of NaNbO3-BaTiO3 lead-free relaxor ferroelectrics. Appl. Phys. Lett. 2016, 108, 232904. [Google Scholar] [CrossRef] [Green Version]
  38. Jin, L.; Huo, R.; Guo, R.; Li, F.; Wang, D.; Tian, Y.; Hu, Q.; Wei, X.; He, Z.; Yan, Y.; et al. Diffuse phase transitions and giant electrostrictive coefficients in lead-free Fe3+-doped 0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Ca0.3)TiO3 ferroelectric ceramics. ACS Appl. Mater. Interfaces 2016, 8, 31109–31119. [Google Scholar] [CrossRef]
  39. Nomura, S.; Uchino, K. Electrostrictive effect in Pb(Mg1/3Nb2/3)O3-type materials. Ferroelectrics 2017, 41, 117–132. [Google Scholar] [CrossRef]
Materials 15 01789 g001 550
Figure 1. XRD patterns of BTS-BCT-xBF ceramics sintered with (a) MWS and (b) CS; enlarged XRD patterns with multi peak fitting of BTS-BCT-xBF ceramics with (c) x = 0.002, (d) x = 0.004 sintered by MWS; enlarged XRD patterns with multi-peak fitting of BTS-BCT-xBF ceramics with (e) x = 0.002, (f) x = 0.004 sintered by CS.
Figure 1. XRD patterns of BTS-BCT-xBF ceramics sintered with (a) MWS and (b) CS; enlarged XRD patterns with multi peak fitting of BTS-BCT-xBF ceramics with (c) x = 0.002, (d) x = 0.004 sintered by MWS; enlarged XRD patterns with multi-peak fitting of BTS-BCT-xBF ceramics with (e) x = 0.002, (f) x = 0.004 sintered by CS.
Materials 15 01789 g001
Materials 15 01789 g002 550
Figure 2. (a–f) εr-T curves from −80 °C to 120 °C of BTS-BCT-xBF ceramics sintered with MWS and CS. (g,h) Phase diagrams of BTS-BCT-xBF ceramics sintered with MWS and CS, respectively.
Figure 2. (a–f) εr-T curves from −80 °C to 120 °C of BTS-BCT-xBF ceramics sintered with MWS and CS. (g,h) Phase diagrams of BTS-BCT-xBF ceramics sintered with MWS and CS, respectively.
Materials 15 01789 g002
Materials 15 01789 g003 550
Figure 3. Plots of ln(1/εr − 1/εm) versus ln(T − Tm) of BST-BCT-xBF ceramics with MWS and CS, (a) x = 0.002, (b) x = 0.004, (c) x = 0.012.
Figure 3. Plots of ln(1/εr − 1/εm) versus ln(T − Tm) of BST-BCT-xBF ceramics with MWS and CS, (a) x = 0.002, (b) x = 0.004, (c) x = 0.012.
Materials 15 01789 g003
Materials 15 01789 g004 550
Figure 4. Surface morphology images of the BTS-BCT-xBF ceramics sintered by (a–d) MWS and (e–h) CS, (i) Grain sizes of MWS and CS BTS-BCT-xBF ceramics.
Figure 4. Surface morphology images of the BTS-BCT-xBF ceramics sintered by (a–d) MWS and (e–h) CS, (i) Grain sizes of MWS and CS BTS-BCT-xBF ceramics.
Materials 15 01789 g004
Materials 15 01789 g005 550
Figure 5. P-E and S-E loops of (a) MWS and (b) CS sintered BTS-BCT-xBF ceramics.
Figure 5. P-E and S-E loops of (a) MWS and (b) CS sintered BTS-BCT-xBF ceramics.
Materials 15 01789 g005
Materials 15 01789 g006 550
Figure 6. (a) Pr, (b) Ec, (c) Spos, (d) εr, (e) tan δ, and (f) d33 of BTS-BCT-xBF ceramics sintered with MWS and CS.
Figure 6. (a) Pr, (b) Ec, (c) Spos, (d) εr, (e) tan δ, and (f) d33 of BTS-BCT-xBF ceramics sintered with MWS and CS.
Materials 15 01789 g006
Materials 15 01789 g007 550
Figure 7. (a) P-E loops, energy storage performance of (b) MWS and (c) CS of BTS-BCT-xBF ceramics with x = 0.012.
Figure 7. (a) P-E loops, energy storage performance of (b) MWS and (c) CS of BTS-BCT-xBF ceramics with x = 0.012.
Materials 15 01789 g007
Materials 15 01789 g008 550
Figure 8. S-P loops of BST-BCT-xBF ceramics sintered with (a) MWS and (b) CS.
Figure 8. S-P loops of BST-BCT-xBF ceramics sintered with (a) MWS and (b) CS.
Materials 15 01789 g008
Table
Table 1. Density of BTS-BCT-xBF ceramics sintering by MWS and CS.
Table 1. Density of BTS-BCT-xBF ceramics sintering by MWS and CS.
xSintering MethodDensity (g/cm3)Sintering MethodDensity (g/cm3)
0.002CS5.8005 MW5.8364
0.0045.8285 5.9100
0.0065.7959 5.8653
0.0085.7644 5.8435
0.0105.7721 5.8195
0.0125.80595.8065
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Wang, T.; Ma, J.; Wu, B.; Wang, F.; Wang, S.; Chen, M.; Wu, W. Structure and Electrical Properties of Microwave Sintered BTS-BCT-xBF Lead-Free Piezoelectric Ceramics. Materials 2022, 15, 1789. https://doi.org/10.3390/ma15051789

AMA Style

Wang T, Ma J, Wu B, Wang F, Wang S, Chen M, Wu W. Structure and Electrical Properties of Microwave Sintered BTS-BCT-xBF Lead-Free Piezoelectric Ceramics. Materials. 2022; 15(5):1789. https://doi.org/10.3390/ma15051789

Chicago/Turabian Style

Wang, Tao, Jian Ma, Bo Wu, Fenghua Wang, Shiyu Wang, Min Chen, and Wenjuan Wu. 2022. "Structure and Electrical Properties of Microwave Sintered BTS-BCT-xBF Lead-Free Piezoelectric Ceramics" Materials 15, no. 5: 1789. https://doi.org/10.3390/ma15051789

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

Article Metrics

Back to TopTop