Piezoelectric Properties of 2.0%Sm-0.25Pb(Mg1/3Nb2/3)O3-0.75Pb(Zr1-xTix)O3 Ceramics Prepared by One-step Method
WANG Yuequn1, XIANG Guanglei1,*, GAO Liang1, WANG Yiping2
1 Hangzhou Applied Acoustics Research Institute, Hangzhou 310023, China 2 State Key Laboratory of Mechanics and Control of Mechanical Structures, Nanjing University of Aeronautics & Astronautics, Nanjing 210016, China
Abstract: Niobium magnesium-lead zirconate titanate (Pb(Mg1/3Nb2/3)O3-Pb(Zr, Ti)O3, PMN-PZT) ceramics are usually prepared by a two-step synthesis method where the MgNb2O6 precursor needs to be synthesized firstly. In industrial production, the two-step synthesis method has relatively low production efficiency and high cost and affects the consistency of product performance. In this work, 2.0mol%Sm-0.25Pb-(Mg1/3Nb2/3)O3-0.75Pb(Zr1-xTix)O3 (Sm-PMN-PZT) piezoelectric ceramics with high density and high piezoelectric properties were prepared by a one-step synthesis method with high efficiency and low cost. In the range of x=0.52—0.53, the morphotropic phase boundaries (MPBs) with the coexistence of rhombohedral (R) and tetragonal phases (T) were constructed. Introduction of Sm3+ enhances the heterogeneity of local polar structures, decreases the potential barrier required for the transition of R-T phase under external electric field (Eex), minimizes the curvature of the free energy curve and finally improves the piezoelectric properties. The ceramic at x=0.525 presents the best comprehensive electrical performance, such as piezoelectric coefficient d33=645 pC/N, the planar electromechanical coupling coefficient kp of 0.657, the relative dielectric constant εr of 3 110, the dielectric loss tanδ of 1.78%, and the ferroelectric Curie temperature TC of 242 ℃. Based on Rayleigh’s law analysis, it has been found that the ceramic at x=0.525 achieves the high piezoelectricity due to its intrinsic response of lattice contribution and reversible domain wall movement, and extrinsic piezoelectric response of irreversible domain wall movement both being enhanced.
1 Damjanovic D. Reports on Progress in Physics, 1998, 61(9), 1267. 2 Zhang S J, Li F, Jiang X N, et al. Progress of Materials Science, 2015, 68, 1. 3 Smolensky G, Isupov V, Granovaskaya A, et al. Journal of Applied Physics, 1954, 25(6), 809. 4 Topolov V Y, Ye Z G. Physical Review B, 2004, 70, 094113. 5 Joe K, Mark L, Chutima T, et al. Journal of the American Ceramic Society, 1997, 80(4), 957. 6 Noheda B, Cox D E, Shirane G, et al. Physical Review B, 2002, 66(5), 054104. 7 Chen J, Chan H M, Harmer M P. Journal of the American Ceramic Society, 1989, 72, 593. 8 Li F, Lin D B, Chen Z B, et al. Nature Materials, 2018, 17, 349. 9 Zheng K, Quan Y, Zhuang J, et al. Journal of the European Ceramic Society, 2021, 41(4), 2458. 10 Guo Q H, Hou L T, Li F, et al. Journal of the American Ceramic Society, 2019, 102, 7428. 11 Dong C, Liang R H, Zhou Z Y, et al. Journal of Inorganic Materials, 2021, 36(12), 1270. 12 Panigrahi S C, Das P R, Padhee R, et al. Ferroelectrics, 2018, 524(1), 14. 13 Li K, Sun E, Zhang Y, et al. Journal of Materials Chemistry C, 2021, 9(7), 2426. 14 Guo Q H, Li F, Xia F Q, et al. ACS Applied Materials & Interfaces, 2019, 11(46), 43359. 15 Wang Y Q, Xiang G L, Gao L. Bulletin of the Chinese ceramic Society, 2022, 41(4), 1433(in Chinese). 汪跃群, 项光磊, 高亮. 硅酸盐通报, 2022, 41(4), 1433. 16 Zhang J, Wang R X, Sun L, et al. Journal of the American Ceramic Society, 2019, 102, 1866. 17 Kalema V, Shih W Y, Shih W H. Ceramics International, 2018, 44, 2835. 18 Wang H L, Zhang F F, Yu C, et al. Ceramics International, 2021, 47, 12284. 19 Sakaki C, Nwwalkar B L, Komarneni S, et al. Japanese Jounral of Applied Physics, 2001, 40(12), 6907. 20 Eitel R E, Shrout T R, Randall C A. Journal of Applied Physics, 2006, 99(12), 177. 21 Li F, Zhang S, Damjanovic D, et al. Advanced Functional Materials, 2018, 28(37), 1801504.