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

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Front. Mater. Sci. ›› 2014, Vol. 8 ›› Issue (2) : 165-175. DOI: 10.1007/s11706-014-0245-9
RESEARCH ARTICLE
RESEARCH ARTICLE

Origin of high mechanical quality factor in CuO-doped (K, Na)NbO3-based ceramics

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Abstract

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.

Keywords

lead-free piezoelectric ceramic / (K, Na)NbO3 (KNN) / mechanism of hardening effect / mechanical quality factor Qm / domain stabilization

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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. Front. Mater. Sci., 2014, 8(2): 165‒175 https://doi.org/10.1007/s11706-014-0245-9

References

[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, . Loss mechanisms and high power piezoelectrics. Journal of Materials Science, 2006, 41(1): 217-228
[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, . Perspective on the development of lead-free piezoceramics. Journal of the American Ceramic Society, 2009, 92(6): 1153-1177
[5]
Xiao D Q, Wu J G, Wu L, . Investigation on the composition design and properties study of perovskite lead-free piezoelectric ceramics. Journal of Materials Science, 2009, 44(19): 5408-5419
[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, . Microstructural evolution of crystalline-oriented (K0.5Na0.5)NbO3 piezoelectric ceramics with a sintering aid of CuO. Journal of the American Ceramic Society, 2006, 89(6): 1951-1956
[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, . Microstructure and piezoelectric properties of the CuO-added (Na0.5K0.5)(Nb0.97Sb0.03)O3 lead-free piezoelectric ceramics. Journal of Applied Physics, 2008, 104(3): 034103 (7 pages)
[19]
Su S, Zuo R, Wang X, . Sintering, microstructure and piezoelectric properties of CuO and SnO2 co-modified sodium potassium niobate ceramics. Materials Research Bulletin, 2010, 45(2): 124-128
[20]
Park B C, Hong I K, Jang H D, . Highly enhanced mechanical quality factor in lead-free (K0.5Na0.5) NbO3 piezoelectric ceramics by co-doping with K5.4Cu1.3Ta10O29 and CuO. Materials Letters, 2010, 64(14): 1577-1579
[21]
Li E, Kakemoto H, Wada S, . Enhancement of Qm by co-doping of Li and Cu to potassium sodium niobate lead-free ceramics. IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, 2008, 55(5): 980-987
[22]
Park H Y, Seo I T, Choi J H, . Low-temperature sintering and piezoelectric properties of (Na0.5K0.5)NbO3 lead-free piezoelectric ceramics. Journal of the American Ceramic Society, 2010, 93(1): 36-39
[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, . Shear-mode piezoelectric properties of modified-(K,Na)NbO3 ceramics for “hard” lead-free materials. Journal of the American Ceramic Society, 2010, 93(9): 2519-2521
[26]
Lv Y G, Wang C L, Zhang J L, . Modified (K0.5Na0.5)(Nb0.9Ta0.1)O3 ceramics with high Qm. Materials Letters, 2008, 62(19): 3425-3427
[27]
Matsubara M, Yamaguchi T, Sakamoto W, . Processing and piezoelectric properties of lead-free (K,Na)(Nb,Ta)O3 ceramics. Journal of the American Ceramic Society, 2005, 88(5): 1190-1196
[28]
Yang M-R, Tsai C-C, Hong C-S, . Piezoelectric and ferroelectric properties of CN-doped K0.5Na0.5NbO3 lead-free ceramics. Journal of Applied Physics, 2010, 108(9): 094103 (5 pages)
[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, . Processing and piezoelectric properties of (Na0.5K0.5)0.96Li0.04(Ta0.1Nb0.9)1-xCuxO3-3x/2 lead-free ceramics. Journal of the American Ceramic Society, 2008, 91(3): 914-917

Acknowledgements

This work was supported by the National Natural Science Foundation of China (NSFC; Grant Nos. 11305152, 51272164, 50772068 and 50972095) and Foundation of Doctor Training Program in University and College in China (Grant Nos. 20030610035 and 20080610020).

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2014 Higher Education Press and Springer-Verlag Berlin Heidelberg
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