不同晶粒取向钛酸铋陶瓷的铁电和压电性能

用固相烧结工艺制备了不同取向率(I)的Bi4Ti3O12(BTO)多晶陶瓷样品.在相同的烧结温度(1140℃),BTO样品的I随烧结时间(2～20h)的增加出现了先升高后降低的变化趋势,最大值达89.9%.样品的铁电和压电性能均与样品的I有关,在α/(b)择优取向的BTO样品的铁电和压电性能都随样品I的升高而改善,其2倍剩余极化强度(Pr)和压电系数(d33)分别达到53.4μC/cm2和22.2pC/N;c取向样品的2Pr和d33则随着取向率的升高而降低.     

(1-x)Na0.5 Bi0.5 TiO3-xNaNbO3系无铅压电陶瓷的机电性能

采用传统陶瓷的制备方法,制备了(1-x)Na0.5Bi0.5TiO3-xNaNbO3(r=0～0．08)压电陶瓷。X射线衍射分析表明：所研究的组成均能够形成纯钙钛矿(ABOx)型固溶体。不同频率下陶瓷材料的介电常数-温度曲线显示该体系材料具有典型的弛豫铁电体特征,且随着x的增加,其弛豫性特征愈明显。室温下陶瓷材料的饱和电滞回线表明：所研究组成均为铁电体．材料的剩余极化强度P1在x=0．02时具有最大值。检测了不同组成陶瓷的雎电性能,发现材料的压电常数d33和平面机电耦合系数Kp随着x值的增加先增加后降低,在x=0．02时．陶瓷的d33=88pC／N,Kp=0．1792,为所研究组成中的最大值．材料的介电常数εI3/ε0和介电损耗tanδ则随x值的增加而增加。     

无铅压电陶瓷材料的研究现状

本文综述了近年来国内外无铅压电陶瓷材料方面的研究进展,重点介绍了钛酸钡基、铋层状结构、钛酸铋钠基、碱金属铌酸盐系以及钨青铜结构无铅压电陶瓷体系的研究现状,并对无铅压电陶瓷的发展作了展望。     

无铅压电陶瓷的电学和力学性能(英文)

利用常规烧结方法制备出了多种A位离子掺杂的钛酸铋纳[(Bi1/2Na1/2)TiO3,BNT]无铅压电陶瓷。对BNT基陶瓷的电学性能和力学性能进行了研究。在(1-x)(Bi1/2Na1/2)0.900Ba0.088Sr0.012TiO3-x(Bi1/2K1/2)TiO3(x=0-0.14)陶瓷体系中,当x=0.10时,可获得最大压电常数(168 pC/N)。在1 kHz,这种陶瓷的介电常数、介电损耗和平面机电耦合系数分别为1 221,0.036 1和0.228 1。Curie温度随x的增加先增加,当x=0.12时,达到最高值(300℃),随后,当x值进一步增加,Curie温度降低。该种无铅压电陶瓷的Vickers硬度和断裂韧性分别为5.0 GPa和2.0 MPa.m1/2,均高于Pb(Zr,Ti)O3陶瓷。     

La3+掺杂钛酸铋钠基无铅陶瓷的压电性能与介电弛豫行为

采用冷等静压成型和密闭烧结工艺,制备了具有微晶结构的稀土离子La3+掺杂0.9TNa0.5Bi0.5TiO3-0.03K0.5Na0.5NbO3基无铅压电陶瓷体系.研究了该体系陶瓷的相结构,显微结构与介电、压电性能.结果表明:在掺杂范围内(0.015≤x≤0.105),La3+可完全固溶进陶瓷晶格形成单一的钙钛矿相.采用等静压成型工艺可明显改善陶瓷的显微结构,使晶粒细化,进而提高材料的压电性能.该陶瓷具有弥散相变和频率色散特征,为典型的弛豫型铁电体.随着La3+掺杂量的增加,材料的铁电-反铁电相变温度下降,Curie温度提高,相对介电常数、介电损耗和压电常数逐渐减小,弛豫特征愈明显.     

钛酸钡系无铅压电陶瓷的研究进展

钛酸钡（BaTiO3）压电陶瓷具有优异的电性能和低污染性，长期以来是人们重点研究的对象。本文综述了近年来BaTiO3系无铅压电陶瓷研究开发的几种体系与进展，着重介绍了BT--BNT和BT-BKT二元系无铅压电陶瓷的结构及性能。同时对BaTiO3系无铅压电陶瓷的发展趋势作了评述。     

无铅压电陶瓷材料研究现状

随着人们环保意识的增强，无铅压电陶瓷材料的研究和应用已日益引起人们的关注。文中综合介绍了铋层状材料和钛酸铋钠基无铅材料的压电特性，总结了各种添加剂对其压电性能的影响机理和规律，介绍了当前以各种工艺对其微观结构和压电性能改进的研究成果，并对2种材料的应用前景进行了展望。     

压电陶瓷PZN-PZT对压电复合材料性能的影响

本研究采用固相烧结法合成了PZN-PZT压电陶瓷粉体,并用XRD分析了其晶相组成。将PZN-PZT陶瓷粉体与PVDF复合,制备出PZN-PZT/PVDF0-3型压电复合材料,研究了陶瓷质量分数对复合材料铁电性、介电性及压电性的影响。结果表明,复合材料的铁电性、介电性和压电性能随陶瓷含量的增加而增强,当陶瓷含量为90%时,复合材料的剩余极化强度Pr达到5.27μC·cm-2,矫顽场EC为76kV·cm-1,介电常数εr为188,介电损耗tanδ为0.065,压电常数d33则达到33.4pC/N。     

Na0.5Bi0.5TiO3-K0.5Bi0.5TiO3系无铅压电陶瓷的极化工艺研究

主要研究了极化电场,极化时间和极化温度等工艺参数对Na0.5Bi0.5TiO3-K0.5Bi0.5TiO3系无铅压电陶瓷介电和压电性能的影响。结果表明:极化电场和极化温度对压电陶瓷的介电、压电性能影响较大,而极化时间则影响较小。适宜的极化电场是3～3.5kV/mm,极化温度70～80℃,极化时间为10～15min。     

BiFeO_3掺杂改性铌酸钾钠无铅压电陶瓷

采用传统固相法制备了(1–x)(K0.5Na0.5)NbO3-xBiFeO3[(1–x)KNN-xBF]无铅压电陶瓷,研究了不同BF含量(x=0,0.175%,0.5%,1%,2%,3%,摩尔分数)样品的物相组成、显微结构及电性能。结果表明:当x≤3%时,得到了纯钙钛矿结构的(1–x)KNN-xBF陶瓷。与纯KNN相比,在0x≤1%时,(1–x)KNN-xBF样品的密度(ρ)、压电常数(d33)、平面机电耦合系数(kp)和机械品质因子(Qm)都显著增大;当1%x≤3%时,ρ,d33,kp和Qm又迅速降低;在x=1%时达到最大值。x=1%时,(1-x)KNN–xBF材料的综合性能最好,其中ρ=4.42g/cm3,d33=172pC/N,kp=0.45,介电损耗tanδ=0.021,相对介电常数εr=759和Qm=138;同时表现出较好的抗老化性能。     

铋层状结构铁电材料的性能与改性研究

铋层状材料具有优良的铁电性能,本文介绍了铋层状材料的结构及其特点,并且综述了其铁电性能(疲劳性能、压电性能)的研究现状、存在的问题.介绍了几种铋层状结构材料改性的工艺措施(热铸法、模板定向生长技术、掺杂).     

(Na1-xKx)0.5Bi0.5TiO3系的离子挥发性研究

利用固相法制备了(Na1-xKx)0.5Bi0.5TiO3系压电陶瓷,研究其中Bi3 、Na 、K 离子的挥发对其性能的影响。研究结果表明Bi3 的挥发性对样品的性能影响较大,而Na 、K 离子相对较小。     

BNKT-xLaFeO3压电陶瓷的性能与微结构

采用传统固相法合成了(1-x)Bi0.5(Na0.8K0.2)0.5TiO3-xLaFeO3无铅压电陶瓷.通过XRD分析,发现该三元体系压电陶瓷均能形成单相钙钛矿结构,并在x=0.005～0.01时范围内具有三方和四方共存结构,为该体系的准同型相界.并研究了该体系压电陶瓷的压电和介电性质.研究结果表明,在室温下该体系表...     

纳米晶钛酸钡陶瓷铁电性能和介电性能的温度依赖性(英文)

研究50nm BaTiO3陶瓷的铁电性能、介电性能的温度依赖性,其介温谱和介电损耗谱具有明显的弥散相变特征,当频率为1kHz时计算得到弥散指数γ为1.60。不同温度下的介电常数–电场强度(ε–E)曲线显示,介电异常发生在110～120℃的温度范围内,110℃时的介电可调性为20.2%,介电损耗小于0.02。压电位移曲线计算得到50nm BaTiO3陶瓷的压电系数d33为45pm/V。     

掺杂三氧化二锑的钛酸铋钠钾陶瓷的显微结构和电学性能

采用固相合成工艺制备了（1–x）[0.82Bi0.5Na0.5TiO3–0.18Bi0.5K0.5TiO3]–xSb2O3（BNKT–xSb）压电陶瓷,研究了Sb2O3掺杂对BNKT陶瓷的显微结构和电学性能的影响规律。研究表明：Sb2O3掺杂量x小于0.020时,不改变基体的钙钛矿结构,且Sb具有可变化合价,能形成＂施主＂和＂受主＂2种掺杂而起到＂软化＂或＂硬化＂的作用。当Sb2O3掺杂量x≤0.005时,其压电系数d33随Sb2O3掺杂量的增加而增大,此时Sb2O3表现出了＂软化＂的特征;当Sb2O3掺杂量x〉0.005时,d33降低,从而又表现出了＂硬化＂的特性;当Sb2O3掺杂≥0.010时,诱使陶瓷室温下反铁电微畴的形成,导致铁电性和压电性的骤减。     

A/B位离子掺杂BiFeO3纳米薄膜的微结构与铁电性能

采用化学溶液法结合层层旋涂退火工艺,在掺氟氧化锡导电玻璃基片上制备了BiFe_0.95Mn_0.05O₃和Bi_0.9Nd_0.1FeO₃纳米晶铁电薄膜,并分析比较了其微结构和铁电性能。结果表明:2组分样品均为单相多晶钙钛矿结构,晶粒细小均匀,表面平整,结构致密。两薄膜均获得了饱和电滞回线,且BiFe_0.95Mn_0.05O₃薄膜具有向上的择优取向极化和更优异的铁电性能,其剩余极化强度(Pr)达60mC·cm^–2,在1~50 k Hz频率范围与25~200℃温度区间内铁电极化响应稳定,保持时间长达1′10³ s工作与反复极化翻转高达1′10⁹次表现出优异的电荷保持力和抗疲劳稳定性。     

Effect of Aliovalent Substituents on the Ferroelectric Properties of Modified Barium Titanate Ceramics - Relaxor Ferroelectric Behavior

Structure–property relationships were investigated to reveal the generic influence of various substituents on ferroelectric BaTiO₃. Compositional modifications of ferroelectric BaTiO₃ were systematically investigated for La³⁺ and Nb⁵⁺ substituents. A generic influence of charged point defects in breaking down the ferroelectric domains into polar clusters was demonstrated. In both types of modified BaTiO₃, relaxor ferroelectric behavior was induced for higher concentrations of substituents.     

Dielectric and Electromechanical Properties of Textured Niobium-Doped Bismuth Titanate Ceramics

Textured Nb-doped bismuth titanate ceramics (Bi₄Ti_{3− x /5}- Nb _{x /5}O₁₂, where x = 0.02) were fabricated by templated grain growth. It was found that the use of a fine precursor powder led to enhanced densification of the ceramic, while Nb doping reduced electrical conduction and dielectric loss, which enabled poling at high temperatures and high electric fields. Sintered tapes showed anisotropic dielectric and piezoelectric properties when measured parallel and perpendicular to the casting plane (e.g., the remanent polarization differed by more than a factor of 15 in the two directions). The piezoelectric constant parallel to the casting plane of the tape was ∼30 pC/N, or ∼77% of the single-crystal value. Thermal depoling studies demonstrated that high-temperature piezoelectric applications are possible up to ∼450°C in textured, doped bismuth titanate.     

中温烧结PSBN系统铁电陶瓷结构和性能的研究

本文研究了中温烧结PbO-SrO-BaO-Nb2O5(PSBN)系统铁电陶瓷介电性能.通过XRD分析确定了主晶相为具有钨青铜结构的Pb0.7Ba0.3Nb2O6(PBN)、Ba0.27Sr0.75Nb2O5.78(BSN);分析了添加剂MnCO3、TiO2、Fe2O3、(MgCO3)4.Mg(OH)2.5H2O对PSBN系统铁电陶瓷介电性能的影响.由于这些添加剂的作用使该系统铁电陶瓷介电系数提高,居里区拓宽并向低温方向移动,绝缘电阻提高,损耗降低,制得高介(ε=4300±200)X7R瓷料.     

Thermally‐induced phase transformations in Na0.5Bi0.5TiO3–KNbO3 ceramics

The structures and functional properties of Na_0.5Bi_0.5TiO₃–xKNbO₃ (NBT‐xKN) solid solutions, with x in the range from 0.01 to 0.09, were investigated using a combination of high‐resolution synchrotron X‐ray powder diffraction (SXPD) and ferroelectric property measurements. For low KN contents, an irreversible transformation from cubic to rhombohedral phases was observed after the application of a high electric field, indicating that the polar nanoregions (PNRs) in the unpoled state can be transformed into metastable long‐range ordered ferroelectric domains in the poled state. In contrast, the near‐cubic phase of the unpoled ceramics was found to be remarkably stable and was retained on cooling to a temperature of ?175°C. Upon heating, the field‐induced metastable ferroelectric rhombohedral phase transformed back to the nanopolar cubic state at the structural transformation temperature, T_ST, which was determined as approximately 225°C and 125°C for KN contents of 3% and 5% respectively. For the field‐induced rhombohedral phase in the poled specimens, the pseudo‐cubic lattice parameter, a_p, exhibited an anomalous reduction while the inter‐axial angle increased towards a value of 90° on heating, resulting in an overall increase in volume. The observed structural changes were correlated with the results of temperature‐dependent dielectric, ferroelectric and depolarization measurements, enabling the construction of a phase diagram to define the stable regions of the different ferroelectric phases as a function of composition and temperature.