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PZT基陶瓷铁电-反铁电相界处各向异性的研究 被引量:6
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作者 董显林 孙大志 王永令 《无机材料学报》 SCIE EI CAS CSCD 北大核心 1995年第2期193-198,共6页
本文研究了两个以PZT瓷为基的系统:PZT(Nb)和PSZT陶瓷在铁电-反铁电相界区域的压电和机电耦合等性能.结果表明,PZT基陶瓷在该相界处具有高Kt和低Kp的性质.压电和机电耦合各向异性也比准同型相界要高,|d3... 本文研究了两个以PZT瓷为基的系统:PZT(Nb)和PSZT陶瓷在铁电-反铁电相界区域的压电和机电耦合等性能.结果表明,PZT基陶瓷在该相界处具有高Kt和低Kp的性质.压电和机电耦合各向异性也比准同型相界要高,|d33/d31|>5.5,Kt/Kp>3.0.借助于电场诱导AF—F相变和反铁电双子晶格间的强耦合作用,对此现象作了较好解释. 展开更多
关键词 PZT陶瓷 各向异性 FA相界 压电陶瓷
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垂直铁电反铁电相界的PSZT陶瓷材料的相变研究
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作者 陈智明 练静予 王永令 《无机材料学报》 SCIE EI CAS CSCD 北大核心 1989年第2期112-118,共7页
利用 Goldschmidt 因子计算具有垂直铁电(F)反铁电(AF)相界的 PSZT 三元系材料,并由实验证实。透射电镜观察到 F、AF 两相在同一晶粒内共存。用电滞回线、热释电、介电等方法测试了该相界附近材料的宏观电性能,研究了它们在外电场和静... 利用 Goldschmidt 因子计算具有垂直铁电(F)反铁电(AF)相界的 PSZT 三元系材料,并由实验证实。透射电镜观察到 F、AF 两相在同一晶粒内共存。用电滞回线、热释电、介电等方法测试了该相界附近材料的宏观电性能,研究了它们在外电场和静压力下的诱导相变行为及变化规律。 展开更多
关键词 PSZT 陶瓷材料 相变 铁电 反铁电
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Ferroelectric domains and phase transition of sol-gel processed epitaxial Sm-doped BiFeO_(3)(001)thin films 被引量:3
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作者 Zhen Zhou Wei Sun +3 位作者 Zhenyu Liao Shuai Ning Jing Zhu Jing-Feng Li 《Journal of Materiomics》 SCIE EI 2018年第1期27-34,共8页
BiFeO_(3),a room-temperature multiferroic material,has recently been increasingly applied as a potential lead-free piezoelectric material due to its large piezoelectricity achieved by doping.In this work,12%Smdoped Bi... BiFeO_(3),a room-temperature multiferroic material,has recently been increasingly applied as a potential lead-free piezoelectric material due to its large piezoelectricity achieved by doping.In this work,12%Smdoped BiFeO_(3)epitaxial thin films were fabricated on Nb-doped SrTiO_(3)(001)single crystal substrates via sol-gel method.The epitaxy was verified by reciprocal space mapping(RSM)and transmission electron microscope(TEM).The TEM results indicated the coexistence of R3c and Pbam phases in the film.The domains and piezoelectric properties from room temperature to 200℃were characterized by piezoresponse force microscopy(PFM).Domains became active from 110℃to 170℃,and domain configurations changed obviously.A partially fading piezoresponse indicated the emergence of antiferroelectric Pbam.The in-situ domain analysis suggested that the phase transition was accompanied by domain wall motion.Switching spectroscopy PFM(SS-PFM)was further conducted to investigate the piezoresponse during the phase transition.Anomalous responses were found in both ON and OFF states at 170℃,and the film exhibits typical antiferroelectric behavior at 200℃,implying that the completion of phase transition and structure turned to the Pbam phase.This work revealed the origin of the high piezoresponse of Sm-doped BiFeO_(3)thin films at the morphotropic phase boundary(MPB). 展开更多
关键词 BiFeO_(3) Piezoresponse force microscopy Morphotropic phase boundary phase transition antiferroelectric
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Nanostructures formation in ferroelectrics in the process of phase transformation
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作者 V.Ishchuk N.Spiridonov V.Sobolev 《Journal of Advanced Dielectrics》 CAS 2014年第4期32-41,共10页
Received 26 June 2014;Revised 13 October 2014;Accepted 20 October 2014;Published 12 November 2014 Inhomogeneous states caused by the coexistence of the ferroelectric(FE)and antiferroelectric(AFE)phases in lead–zircon... Received 26 June 2014;Revised 13 October 2014;Accepted 20 October 2014;Published 12 November 2014 Inhomogeneous states caused by the coexistence of the ferroelectric(FE)and antiferroelectric(AFE)phases in lead–zirconate–titanate based solid solutions have been investigated.It has been found that the domains of the FE and AFE phases with sizes of the order of 20 nm to 30 nm coexist in the bulk of the samples due to a small difference in the free energies of these phases.The coherent character of the interphase boundaries(IPBs)leads to the concentration of the elastic stresses along these boundaries.These elastic stresses cause the local decomposition of the solid solution and formation of segregates near the IPBS due to the condition that equivalent positions of the crystal lattice are occupied by the ions with different sizes.The sizes of the segregates formed in this way are of the order 8 nm to 15 nm.Some physical effects caused by the presence of these segregate nanostructures are analyzed and discussed. 展开更多
关键词 FERROELECTRICS antiferroelectricS phase transitions phase coexistence interdomain boundaries local decomposition of solid solutions
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(Pb_(0.97)La_(0.02))(Zr_(0.65)Sn_(0.35-x)Ti_x)O_3反铁电陶瓷的热膨胀性质 被引量:1
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作者 刘鹏 徐卓 姚熹 《物理学报》 SCIE EI CAS CSCD 北大核心 2003年第9期2314-2318,共5页
在 - 10 0— 2 0 0℃温度范围内 ,测量了 (Pb0 .97La0 .0 2 ) (Zr0 .6 5Sn0 .35-xTix)O3(PZST ,0 1≤x≤ 0 14 )反铁电陶瓷的热膨胀性质 .实验结果表明 ,组分在 0 1≤x≤ 0 12的试样室温下为反铁电 (AFEt)四方相 ,热膨胀系数 (α)... 在 - 10 0— 2 0 0℃温度范围内 ,测量了 (Pb0 .97La0 .0 2 ) (Zr0 .6 5Sn0 .35-xTix)O3(PZST ,0 1≤x≤ 0 14 )反铁电陶瓷的热膨胀性质 .实验结果表明 ,组分在 0 1≤x≤ 0 12的试样室温下为反铁电 (AFEt)四方相 ,热膨胀系数 (α)在低温段发生“弯曲” ,而变温x射线衍射谱 (XRD)显示材料保持四方相结构 ;当Ti含量在 0 12 5≤x≤ 0 14时 ,室温下是铁电三方相 (FER) ,温度升高时FER →AFEt 相变体积收缩 ,AFEt→立方顺电 (PEc)相变体积增大 ;变温XRD谱证明了材料相结构随温度的转变过程 .用多元复杂化合物存在纳米线度组分非均匀的观点解释了热膨胀性质随Ti含量演化的物理机理 ,并得到了该系统的温度 Ti(x) 展开更多
关键词 热膨胀性质 铁电/反铁电相界 反铁电陶瓷 PZST (Pb0.97La0.02)(Zr0.65Sn0.35-xTix)O3
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(PbBa)(Zr,Sn,Ti)O_3反铁电/弛豫型铁电相界陶瓷的相变与介电、热释电性质
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作者 刘鹏 边小兵 +1 位作者 张良莹 姚熹 《物理学报》 SCIE EI CAS CSCD 北大核心 2002年第7期1628-1633,共6页
通过对 (Pb0 87Ba0 1 La0 0 2 ) (Zr0 6 TixSn0 4 -x)O3(0 0 4≤x≤ 0 2 0 )固溶体的介电和偏压热释电性质的研究发现 ,当Ti含量 0 0 4≤x≤ 0 0 7时 ,材料是反铁电四方相 ,而当 0 0 9≤x≤ 0 2 0时 ,材料向弛豫型铁电体转... 通过对 (Pb0 87Ba0 1 La0 0 2 ) (Zr0 6 TixSn0 4 -x)O3(0 0 4≤x≤ 0 2 0 )固溶体的介电和偏压热释电性质的研究发现 ,当Ti含量 0 0 4≤x≤ 0 0 7时 ,材料是反铁电四方相 ,而当 0 0 9≤x≤ 0 2 0时 ,材料向弛豫型铁电体转化 .在温度 Ti含量相图中 ,x =0 0 9附近形成了反铁电 铁电 顺电三相共存点 (Ttr) .该点的相变温度最底 ;对于 0 0 4≤x≤ 0 0 7的反铁电四方相 ,低温下呈现介电弛豫特征 ,并可被外电场诱导为亚稳铁电态 ,温度升高时 ,亚稳铁电→反铁电相变 ,反铁电→顺电相变引起两个热释电流峰 ,偏置电场下峰位和峰强均发生移动 ,在温度 电场相图中也形成了铁电 反铁电 顺电三相点 .从复杂化合物纳米相分离的观点和晶格动力学出发 ,讨论了相变与电学性能随Ti含量 (x)和外电场(E)变化的物理机理 . 展开更多
关键词 反铁电/驰豫型铁电相界 介电性能 偏压热释电性质 铁电-反铁电-顺电三相点 铁电体
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