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Relationship Between Structure and Electric Properties of (0.99–x)BNT–xBKT–0.01KNN Near Morphotropic Phase Boundary
引用本文:叶成根,郝继功,翟继卫.Relationship Between Structure and Electric Properties of (0.99–x)BNT–xBKT–0.01KNN Near Morphotropic Phase Boundary[J].硅酸盐学报,2012,40(3):385-390.
作者姓名:叶成根  郝继功  翟继卫
作者单位:同济大学功能材料研究所,上海,200092
基金项目:国家自然科学基金重点项目
摘    要:研究了三方、四方共存即准同型相界(morphotropic phase boundary,MPB)]附近(0.99–x)Bi0.5Na0.5TiO3–xBi0.5K0.5TiO3–0.01K0.5Na0.5NbO3(0.99–x)BNT–xBKT–0.01KNN,x=0.16~0.23]无铅压电陶瓷的电学性能与其结构之间的变化关系。X射线衍射分析表明,随着x的增大,陶瓷材料相结构由三方相转变为四方相。当x=0.20时,(111)和(200)面衍射峰均形成劈裂峰,标志着该组分的相结构由三方–四方相共同组成,形成MPB区。样品的介电温谱表明,铁电–反铁电转变温度(Td)随着x的增大而减小,但Curie点(TC)并未明显变化。电致应变(S)随着x的增大,呈现先增加后减小的趋势,并在x=0.20时得最大值0.46%,此时动态压电系数约为575 pm/V。电滞回线显示,陶瓷样品的剩余极化强度Pr和矫顽场Ec都随着x的增大而减小,分别由41.5μC/cm2降为15.2μC/cm2和由46.5kV/cm降为15.0kV/cm,并伴随着电滞回线由扁平到束腰的形状变化,呈现从铁电相特性到反铁电相特性的转变过程。

关 键 词:无铅压电陶瓷  准同型相界  电致应变  压电–铁电性能

Relationship Between Structure and Electric Properties of (0.99–x)BNT–xBKT–0.01KNN Near Morphotropic Phase Boundary
YE Chenggen,HAO Jigong,ZHAI Jiwei.Relationship Between Structure and Electric Properties of (0.99–x)BNT–xBKT–0.01KNN Near Morphotropic Phase Boundary[J].Journal of The Chinese Ceramic Society,2012,40(3):385-390.
Authors:YE Chenggen  HAO Jigong  ZHAI Jiwei
Affiliation:(Functional Materials Research Laboratory,Tongji University,Shanghai 200092,China)
Abstract:A relationship between the electric properties and the structure of lead-free ceramics(0.99–x)Bi0.5Na0.5TiO3–xBi0.5K0.5TiO3– 0.01K0.5Na0.5NbO3 (0.99–x)BNT–xBKT–0.01KNN,x = 0.16–0.23] near the region where tetragonal and rhombohedral phase co-existed(morphotropic phase boundary,MPB) was investigated.The analysis by X-ray diffraction indicated the transition from rhombohedral to tetragonal phase as the BKT content x increased.The peak splits of(111) and(200) occurred simultaneously at x = 0.20,indicating the ceramic had a structure of coexistence of rhombohedral and tetragonal phases(viz.formed MPB).The results of dielectric temperature spectra showed that the ferroelectric to anti-ferroelectric transition temperature Td decreased with increasing x,while the Curie point(TC) showed slight changes.The electrostrictive strain(S) firstly increased and then decreased,giving a maxi-mum value of 0.46% at x = 0.20,which equaled to the dynamic piezoelectric coefficients of 575 pm/V.The electric hysteresis loop test exhibited that the remanent polarization Pr and coercive field Ec decreased from 41.5 μC/cm2 to 15.2 μC/cm2 and from 46.5 kV/cm to 15.0 kV/cm,respectively,with increasing x,and the loops showed a transition from ferroelectric properties to anti-ferroelectric properties.
Keywords:lead-free piezoelectric ceramics  morphotropic phase boundary  electrostrictive strain  piezoelectric–ferroelectric property
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