Li Bing, Zheng Ting, Wu Jiagang
Department of Materials Science, Sichuan University, Chengdu 610064, China.
ACS Appl Mater Interfaces. 2021 Aug 11;13(31):37422-37432. doi: 10.1021/acsami.1c10468. Epub 2021 Jul 31.
Bismuth ferrite-barium titanate (BF-BT) ferroelectrics attract attention due to their multifunctional properties and potential applications in high-temperature piezodevices. The thermal depolarization temperature () of BF-BT-based relaxor ferroelectrics has a close correlation with electrical properties, which was only recently discovered and is not well recognized. This work is concerned with the thermal depolarization process in (0.67 - )BF-0.33BT-SZ ferroelectrics with large strain response. Macro-to-local property characterization suggests that the largest electrostrain can be achieved in the critical component ( = 0.02) with the most flexible structure features, which is the transition point from the ferroelectric macrodomain to the relaxor nanodomain. The real-space domain image by piezoresponse force microscopy has revealed that an electric field can transform the labyrinth-like nanodomain into oriented large-size domain. Once the heating temperature is above , the poling-induced large-size oriented domain will transform back to its initial state. Most importantly, the thermally induced domain broken is first established with the conduction and phase transition, as disclosed by temperature dependence of DC resistivity and the pyroelectric coefficient. That is, during the thermal depolarization process, the activation energy () changes from 0.65 eV ( < ) to 1.1 eV ( > ), simultaneously accompanied with the structural transition from the poling-induced unstable ferroelectric state (long-range correlated rhombohedral phase) to the initial relaxor state (short-range correlated pseudo-cubic phase), which may be the driving force for the domain decays above . We believe that the understanding of in BF-BT-based relaxor ferroelectrics can provide some clues for further designing high-performance BF-BT ferroelectrics.
铋铁氧体-钛酸钡(BF-BT)铁电体因其多功能特性以及在高温压电器件中的潜在应用而备受关注。基于BF-BT的弛豫铁电体的热去极化温度()与电学性能密切相关,这一关系直到最近才被发现且尚未得到充分认识。本文研究了具有大应变响应的(0.67 - )BF-0.33BT-SZ铁电体中的热去极化过程。宏观到局部性能表征表明,在具有最灵活结构特征的关键组分( = 0.02)中可实现最大电应变,该组分是从铁电宏畴到弛豫纳米畴的转变点。压电力显微镜的实空间畴图像显示,电场可将迷宫状纳米畴转变为取向大尺寸畴。一旦加热温度高于,极化诱导的大尺寸取向畴将转变回其初始状态。最重要的是,如直流电阻率和热释电系数的温度依赖性所揭示的,热诱导畴破裂首先与传导和相变相关联。也就是说,在热去极化过程中,激活能()从0.65 eV( < )变为1.1 eV( > ),同时伴随着从极化诱导的不稳定铁电态(长程相关菱方相)到初始弛豫态(短程相关准立方相)的结构转变,这可能是高于时畴衰减的驱动力。我们认为,对基于BF-BT的弛豫铁电体中热去极化过程的理解可为进一步设计高性能BF-BT铁电体提供一些线索。