铁电体 BaTi$_{0.8}$Zr$_{0.2}$O$_3$ 中居里温度以上的相变和极簇行为

Oktay Aktas, Francisco Javier Romero, Zhengwang He, Gan Linyu, Xiangdong Ding, José-María Martín-Olalla, Maria-Carmen Gallardo, Turab Lookman
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引用次数: 0

摘要

我们研究了铁电体 BaTi$_{0.8}$Zr$_{0.2}$O$_3$ 在副电区的相变行为。热、极性、弹性和介电性质的温度依赖性表明,在副介电-铁电转变温度 Tc = 292 K 以上存在局部结构。在特征温度 T* ~350 K 以下测量到了非零残余极化,这与介电常数偏离居里-韦斯定律的温度相吻合。共振压电光谱显示,使用小于矫顽力场的场在 Tc 以上进行直流场冷却会导致弹性响应和低于 T* 的残余压电,这可能与铁电中极性纳米结构相关的相干温度一致。所观察到的残余效应归因于极性纳米结构在 Tc 以上的重新定向。
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Phase transition and polar cluster behavior above Curie temperature in ferroelectric BaTi$_{0.8}$Zr$_{0.2}$O$_3$
We study the phase transition behavior of the ferroelectric BaTi$_{0.8}$Zr$_{0.2}$O$_3$ in the paraelectric region. The temperature dependencies of thermal, polar, elastic and dielectric properties indicate the presence of local structures above the paraelectric-ferroelectric transition temperature Tc = 292 K. The non-zero remnant polarization is measured up to a characteristic temperature T* ~350 K, which coincides with the temperature where the dielectric constant deviates from Curie-Weiss law. Resonant Piezoelectric Spectroscopy shows that DC field-cooling above Tc using fields smaller than the coercive field leads to an elastic response and remnant piezoelectricity below T*, which likely corresponds to the coherence temperature associated with polar nanostructures in ferroelectrics. The observed remnant effect is attributed to the reorientation of polar nanostructures above Tc.
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