Dielectric Relaxation and Ferroelectric Imprint

H. Kliem
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引用次数: 1

Abstract

The term imprint is generally used for a special kind of a reversible change in the ferroelectric state. It refers to a time dependent development of the material's resistance against polarization reversal. At the example of P(VDF-TrFE) it is shown that if polarized to the remanent polarization and under a switched off external field the coercive field of the sample's hysteresis loop increases in time, the ferroelectric switching time increases as well, the remanent polarization decreases, and the small signal ac capacitance decreases also. All four effects exhibit a linear behavior on a logarithmic time scale, i.e. they are proportional to log tw, with tw as the waiting time after switching off the external field. A model is developed which relates the four observations. The model is based on a feedback effect between a crystalline phase where the ferroelectric switching takes place and an amorphous or disordered phase with a relaxational polarization response.
介电弛豫和铁电压印
“压印”一词通常用于描述铁电态中一种特殊的可逆变化。它指的是材料抗极化反转阻力的时间依赖性发展。以P(VDF-TrFE)为例,结果表明,当极化到剩余极化时,在关闭外场的情况下,样品磁滞回线的矫顽力场随时间增大,铁电开关时间增大,剩余极化减小,小信号交流电容也减小。所有四种效应在对数时间尺度上都表现出线性行为,即它们与log tw成正比,其中tw为关闭外场后的等待时间。建立了一个将这四种观测结果联系起来的模型。该模型基于发生铁电开关的晶体相与具有弛豫极化响应的非晶态或无序相之间的反馈效应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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