Origin of high mechanical quality factor in CuO-doped (K, Na)NbO3-based ceramics
Wen-Feng LIANG, Ding-Quan XIAO, Jia-Gang WU, Wen-Juan WU, Jian-Guo ZHU
Origin of high mechanical quality factor in CuO-doped (K, Na)NbO3-based ceramics
The origin of a high mechanical quality in CuO-doped (K, Na)NbO3-based ceramics is addressed by considering the correlations between the lattice positions of Cu ions and the hardening effect in K0.48Na0.52+xNbO3--0.01CuO ceramics. The Cu ions simultaneously occupy K/Na and Nb sites of these ceramics with x = 0 and 0.02, only occupy the K/Na site of the ceramics with x = --0.02, and mostly form a secondary phase of the ceramics with x = --0.05. The Cu ions lead to the hardening of ceramics with an increase of EC and Qm by only occupying the K/Na site, together with the formation of double hysteresis loops in un-poled compositions. A defect model is proposed to illuminate the origin of a high Qm value, that is, the domain stabilization is dominated by the content of relatively mobile O2-- ions in the ceramics, which has a weak bonding with CuK/Na defects.
lead-free piezoelectric ceramic / (K, Na)NbO3 (KNN) / mechanism of hardening effect / mechanical quality factor Qm / domain stabilization
[1] |
Gerthsen P, Härdtl K H, Schmidt N A. Correlation of mechanical and electrical losses in ferroelectric ceramics. Journal of Applied Physics, 1980, 51(2): 1131
|
[2] |
Uchino K, Zheng J H, Chen Y H,
|
[3] |
Zhang S, Xia R, Shrout T R. Lead-free piezoelectric ceramics vs PZT? Journal of Electroceramics, 2007, 19(4): 251-257
|
[4] |
Rödel J, Jo W, Seifert K T P,
|
[5] |
Xiao D Q, Wu J G, Wu L,
|
[6] |
Shrout T R, Zhang S J. Lead-free piezoelectric ceramics: Alternatives for PZT? Journal of Electroceramics, 2007, 19(1): 113-126
|
[7] |
Härdtl K H. Electrical and mechanical losses in ferroelectric ceramics. Ceramics International, 1982, 8(4): 121-127
|
[8] |
Lin D, Kwok K W, Chan H L W. Double hysteresis loop in Cu-doped K0.5Na0.5NbO3 lead-free piezoelectric ceramics. Applied Physics Letters, 2007, 90(23): 232903 (3 pages)
|
[9] |
Gao Y, Uchino K, Viehland D. Effects of thermal and electrical histories on hard piezoelectrics: A comparison of internal dipolar fields and external dc bias. Journal of Applied Physics, 2007, 101(5): 054109 (6 pages)
|
[10] |
Lin D, Kwok K W, Wong Lai-wa Chan H.Double hysteresis loop and aging effect in K0.5Na0.5NbO3–K5.4Cu1.3Ta10O9 lead-free ceramics. Journal of the American Ceramic Society, 2009, 92(6): 1362-1365
|
[11] |
Carl K, Hardtl K H. Electrical after-effects in Pb(Ti, Zr)O3 ceramics. Ferroelectrics, 1977, 17(1): 473-486
|
[12] |
Ren X. Large electric-field-induced strain in ferroelectric crystals by point-defect-mediated reversible domain switching. Nature Materials, 2004, 3(2): 91-94
|
[13] |
Zhang L, Ren X. Aging behavior in single-domain Mn-doped BaTiO3 crystals: Implication for a unified microscopic explanation of ferroelectric aging. Physical Review B: Condensed Matter and Materials Physics, 2006, 73: 094121
|
[14] |
Tan Q, Li J, Viehland D. Role of lower valent substituent-oxygen vacancy complexes in polarization pinning in potassium-modified lead zirconate titanate. Applied Physics Letters, 1999, 75(3): 418-420
|
[15] |
Zhang Y, Li J, Fang D. Oxygen-vacancy-induced memory effect and large recoverable strain in a barium titanate single crystal. Physical Review B: Condensed Matter and Materials Physics, 2010, 82: 064103
|
[16] |
Takao H, Saito Y, Aoki Y,
|
[17] |
Wang H-Q, Dai Y-J, Zhang X-W. Microstructure and hardening mechanism of K0.5Na0.5NbO3 lead-free ceramics with CuO doping sintered in different atmospheres. Journal of the American Ceramic Society, 2012, 95(4): 1182-1184
|
[18] |
Park H-Y, Seo I-T, Choi M-K,
|
[19] |
Su S, Zuo R, Wang X,
|
[20] |
Park B C, Hong I K, Jang H D,
|
[21] |
Li E, Kakemoto H, Wada S,
|
[22] |
Park H Y, Seo I T, Choi J H,
|
[23] |
Alkoy E M, Papila M. Microstructural features and electrical properties of copper oxide added potassium sodium niobate ceramics. Ceramics International, 2010, 36(6): 1921-1927
|
[24] |
Lin D, Kwok K W, Chan H L W. Piezoelectric properties and hardening behavior of K5.4Cu1.3Ta10O29-doped K0.5Na0.5NbO3 ceramics. Journal of Applied Physics, 2008, 103(6): 064105 (5 pages)
|
[25] |
Lim J B, Zhang S, Lee H J,
|
[26] |
Lv Y G, Wang C L, Zhang J L,
|
[27] |
Matsubara M, Yamaguchi T, Sakamoto W,
|
[28] |
Yang M-R, Tsai C-C, Hong C-S,
|
[29] |
Körbel S, Marton P, Elsässer C. Formation of vacancies and copper substitutionals in potassium sodium niobate under various processing conditions. Physical Review B: Condensed Matter and Materials<?Pub Caret?> Physics, 2010, 81: 174115
|
[30] |
Shigemi A, Wada T. Evaluations of phases and vacancy formation energies in KNbO3 by first-principles calculation. Japanese Journal of Applied Physics, 2005, 44(11): 8048-8054
|
[31] |
Zhen Y, Li J F. Abnormal grain growth and new core–shell structure in (K,Na)NbO3-based lead-free piezoelectric ceramics. Journal of the American Ceramic Society, 2007, 90(11): 3496-3502
|
[32] |
Zuo R, Ye C, Fang X,
|
/
〈 | 〉 |