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本文引用的文献

1
Temperature dependence of electric-field-induced domain switching in 0.7Pb(MgNb)O-0.3PbTiO single crystal.0.7Pb(MgNb)O-0.3PbTiO 单晶中电场诱导畴切换的温度依赖性
J Alloys Compd. 2012 Jun 25;527:101-105. doi: 10.1016/j.jallcom.2012.02.159.
2
Relaxor-PT single crystals: observations and developments.弛豫铁电单晶：观察与发展。
IEEE Trans Ultrason Ferroelectr Freq Control. 2010 Oct;57(10):2138-46. doi: 10.1109/TUFFC.2010.1670.
3
Elastic, dielectric, and piezoelectric constants of Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3) single crystal poled along [011](c).沿[011](c)极化的Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3)单晶的弹性、介电和压电常数
Appl Phys Lett. 2010 Jul 19;97(3). doi: 10.1063/1.3466906. Epub 2010 Jul 20.
4
Complete set of material constants of Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3)single crystal with morphotropic phase boundary composition.具有准同型相界成分的Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3)单晶的全套材料常数
J Appl Phys. 2009 Oct 1;106(7):74112. doi: 10.1063/1.3243169. Epub 2009 Oct 14.
5
Characterization of Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3) ferroelectric crystal with enhanced phase transition temperatures.具有提高的相变温度的Pb(In(12)Nb(12))O(3)-Pb(Mg(13)Nb(23))O(3)-PbTiO(3)铁电晶体的表征
J Appl Phys. 2008 Sep 15;104(6):64106. doi: 10.1063/1.2978333. Epub 2008 Sep 19.

[001](c)和[011](c)极化的0.33Pb(In(1/2)Nb(1/2))O(3)-0.38Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3)单晶的完整矩阵特性

Complete matrix properties of [001](c) and [011](c) poled 0.33Pb(In(1/2)Nb(1/2))O(3)-0.38Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3) single crystals.

作者信息

Sun Enwei, Zhang Rui, Wu Fengmin, Cao Wenwu

机构信息

Condensed Matter Science and Technology Institute, Harbin Institute of Technology, Harbin 150080, China.

出版信息

J Alloys Compd. 2013 Mar 15;553:267-269. doi: 10.1016/j.jallcom.2012.11.111. Epub 2012 Nov 29.

DOI:10.1016/j.jallcom.2012.11.111
PMID:23378702
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3559011/
Abstract

The elastic, piezoelectric, and dielectric properties of 001 and 011 poled 0.33Pb(In(1/2)Nb(1/2))O(3)-0.38Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3) single crystals have been fully characterized at room temperature, and the temperature and frequency dependence of the dielectric susceptibility ε(33) were also measured. The depoling temperature of this crystal is more than 20 °C higher than that of the corresponding binary 0.71Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3) system. From the measured P-E hysteresis loops, the coercive fields along 001 and 011 directions have been determined to be 6.0 kV/cm and 6.6 kV/cm, respectively, which indicate that these domain engineered ternary relaxor-based ferroelectric single crystals are excellent candidates for high-power applications.

摘要

001和011极化的0.33Pb(In(1/2)Nb(1/2))O(3)-0.38Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3)单晶的弹性、压电和介电性能已在室温下得到充分表征，并且还测量了介电常数ε(33)的温度和频率依赖性。该晶体的退极化温度比相应的二元0.71Pb(Mg(1/3)Nb(2/3))O(3)-0.29PbTiO(3)体系高20℃以上。从测量的P-E磁滞回线可知，沿001和01方向的矫顽场分别确定为6.0 kV/cm和6.6 kV/cm，这表明这些经过畴工程处理的三元弛豫铁电单晶是高功率应用的极佳候选材料。