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首页> 外文期刊>Journal of Materiomics >Polarization reversal via a transient relaxor state in nonergodic relaxors near freezing temperature
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Polarization reversal via a transient relaxor state in nonergodic relaxors near freezing temperature

机译:在接近冰点温度的非遍历弛豫器中通过瞬态弛豫器状态进行极化反转

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Among the unresolved issues in the study of relaxor ferroelectrics is the role of freezing temperature, across which the dynamics of polarization reversal in relaxor ferroelectrics changes. The presence of this freezing temperature is best manifested by the appearance of a double polarization hysteresis loop just above the freezing temperature. Given that the polarization pinching evolving into a double hysteresis starts well below the freezing temperature, there exists a transient temperature regime between the nonergodic and the ergodic relaxor states. To clarify the role of the freezing temperature on the pinching, the polarization reversal near the freezing temperature of relaxor (Pb_(1- x )La_( x ))(Zr_(1- y )T_( y ))_(1- x /4)O_(3) (PLZT) was monitored using three in situ electric field methods: electrocaloric effect, neutron diffraction, and transmission electron microscopy. We demonstrate that the pinching results from a two-step process, 1) domain detexturization in the ferroelectric state and 2) miniaturization of domains. This observation explains the recently reported gap between the depolarization temperature T _(d) and the ferroelectric-to-relaxor transition temperature T _(F-R) in lead-free relaxors. We further show that T _(d) and T _(F-R), which have long been considered identical in lead-based relaxors, are not the same. The current study suggests that the mismatch between T _(d) and T _(F-R) is an inherent feature in both lead-based and lead-free relaxor ferroelectrics.
机译:弛豫铁电学研究中尚未解决的问题之一是冻结温度的作用,冻结温度在弛豫铁电学中的极性反转动力学发生变化。该冷冻温度的存在最好通过在冷冻温度之上出现双极化磁滞回线来最好地证明。考虑到极化收缩发展为双滞后现象的开始时间远低于冰点温度,因此在非遍历和遍历松弛状态之间存在一个瞬态温度状态。为了阐明冻结温度对收缩的作用,在弛豫器的冻结温度附近极化反转(Pb_(1- x)La_(x))(Zr_(1- y)T_(y))_(1- x使用三种原位电场方法监测/ 4)O_(3)(PLZT):电热效应,中子衍射和透射电子显微镜。我们证明了这种收缩是由两步过程引起的:1)铁电态中的畴脱质和2)畴的小型化。该观察结果解释了最近报道的无铅弛张器中的去极化温度T _(d)和铁电-弛豫转变温度T _(F-R)之间的差距。我们进一步表明,T_(d)和T_(F-R)在铅基弛豫器中长期以来被认为是相同的,但并不相同。当前的研究表明,T _(d)和T _(F-R)之间的不匹配是基于铅的无铅弛豫铁电体的固有特征。

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