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Quantitative evaluation of the piezoelectric response of unpoled ferroelectric ceramics from elastic and dielectric measurements: tetragonal BaTiO$_3$

机译:非极化压电响应的定量评估   弹性和介电测量的铁电陶瓷:四方晶系   钛酸钡$ _3 $

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摘要

A method for evaluating the piezoelectric response of unpoled ferroelectricceramics from elastic and dielectric measurements is proposed and tested onBaTiO$_3$. The method is based on the observation that the softening in aferroelectric phase with respect to the paraelectric phase is of piezoelectricorigin. The angular averages of the piezoelectric softening in unpoled ceramicsare calculated for ferroelectric phases of different symmetries. The expressionof the orientational average with the piezoelectric and dielectric constants ofsingle crystal tetragonal BaTiO$_3$ from the literature reproduces well thesoftening of the Young's modulus of unpoled ceramic BaTiO$_3$, after acorrection for the porosity. The agreement is good in the temperature regionsufficiently far from the Curie temperature and from the transition to theorthorhombic phase, where the effect of fluctuations should be negligible, butdeviations are found outside this region, and the reason for this is discussed.This validates the determination of the piezoelectric response by means ofpurely elastic measurements on unpoled samples. The method is indirect and, forquantitative assessments, requires the knowledge of the dielectric tensor. Onthe other hand, it does not require poling of the sample, and therefore isinsensitive to inaccuracies from incomplete poling, and can even be used withmaterials that cannot be poled, for example due to excessive electricalconductivity. While the proposed example of the Young's modulus of a ceramicprovides an orientational average of all the single crystal piezoelectricconstants, a Resonant Ultrasound Spectroscopy measurement of a single unpoledceramic sample through the ferroelectric transition can in principle measureall the piezoelectric constants, together with the elastic ones.
机译:提出了一种通过弹性和介电测量评估非极化铁电陶瓷压电响应的方法,并在BaTiO 3上进行了测试。该方法基于以下观察:相对于顺电相,铁电相中的软化具有压电性。针对不同对称性的铁电相,计算了未极化陶瓷中压电软化的角均值。文献中用单晶四方晶BaTiO $ _3 $的压电常数和介电常数表示的取向平均值可以很好地再现未经极化的陶瓷BaTiO $ _3 $的杨氏模量在校正孔隙度后的软化。在距居里温度足够远的温度区域以及从向斜方晶相转变的温度区域中,该协议是好的,其中波动的影响应可忽略不计,但在该区域之外发现了偏差,并对此进行了讨论,这证实了对通过对未极化样本进行纯弹性测量获得压电响应。该方法是间接的,并且要进行定量评估,需要了解介电张量。另一方面,它不需要样品极化,因此对由于不完全极化而引起的不准确性不敏感,甚至可以与不能极化的材料一起使用,例如由于过高的导电性。虽然提出的陶瓷杨氏模量示例提供了所有单晶压电常数的取向平均值,但通过铁电跃迁对单个非陶瓷样品的共振超声光谱测量原则上可以测量所有压电常数以及弹性常数。

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    Cordero, F.;

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