Issue |
Eur. Phys. J. Appl. Phys.
Volume 66, Number 3, June 2014
|
|
---|---|---|
Article Number | 30101 | |
Number of page(s) | 5 | |
Section | Semiconductors and Devices | |
DOI | https://doi.org/10.1051/epjap/2014140040 | |
Published online | 10 June 2014 |
https://doi.org/10.1051/epjap/2014140040
Synthesis and characterization of Pb(Yb1/2Nb1/2)O3-based high-Curie temperature piezoelectric ceramics
1
School of Information Science and Engineering, School of Materials Science and Engineering, Changzhou University, Changzhou, Jiangsu
213164, P.R. China
2
School of Material Science and Engineering, Jiangsu University, Zhenjiang, Jiangsu
212013, P.R. China
3
Key Laboratory of Inorganic Function Material and Device, Chinese Academy of Sciences, Shanghai
201800, P.R. China
a e-mail: fangbj@sohu.com
b e-mail: dingjn@cczu.edu.cn
Received:
1
February
2014
Revised:
20
April
2014
Accepted:
2
May
2014
Published online:
10
June
2014
xPb(Yb1/2Nb1/2)O3-(1 − x)Pb(Zr0.36Ti0.64)O3 (xPYN-(1 − x)PZT) piezoelectric ceramics were prepared by the conventional ceramic processing via a B-site oxide mixing route. The synthesized xPYN-(1 − x)PZT ceramics exhibit majority of perovskite structure with slight content of impurity, which exhibit typical tetragonal structure with slight orthorhombic distortion depending on compositions. All the xPYN-(1 − x)PZT ceramics exhibit high Curie temperature (TC/Tm), higher than 380 °C, and their dielectric behavior above TC/Tm can be fitted well by the Curie-Weiss law. The xPYN-(1 − x)PZT ceramics exhibit large resistivity, and excellent ferroelectric and piezoelectric properties, which provide promising for the high-power and high-temperature piezoelectric applications. However, electric energy density of the xPYN-(1 − x)PZT ceramics is small due to their nearly rectangular shape of polarization-electric field (P-E) hysteresis loop and early electric displacement saturation, which is not suitable for high energy and power storage applications.
© EDP Sciences, 2014
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