pzn-4.5%pt铁电单晶表面层的常规和高分辨率同步x射线衍射联合研究

W. Chang, L. Lim, P. Yang, H. Moser
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摘要

在室温下,PZN-PT块状单晶的标准XRD谱中,经常观察到与主(002)菱形峰相邻的一个极宽的低2θ峰。为了了解这个低2θ峰的来源和性质,进行了高分辨率同步加速器x射线衍射研究。同步加速器(002)映射与破裂技术一起证实,较低的2θ峰来自抛光诱导的“单斜对称的高应力菱形态”的表面层,在结构上,可以比作一个充满了一系列晶格参数的“早期单斜核”。这些“初期的”单斜核/相在尺寸上是微观的,并且在表层处于强烈的面内压应力下。所有这些都导致了低2θ峰的极端宽。本研究表明,弛豫单晶的变形是由应力诱导的材料从菱形态到其他低对称态的相变引起的。较低的2θ峰,即“初始”单斜面层,对退火和低场极化具有相当的抗性,但当抛光样品在室温下极化到足够高的场(即1.5 kV/mm)时,可以在很大程度上消除。然而,退火后,“初始”单斜面层变得更耐极化,以至于即使在高场极化后,低2θ峰的残余仍然存在。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
COMBINED NORMAL AND HIGH-RESOLUTION SYNCHROTRON X-RAY DIFFRACTION STUDY OF SURFACE LAYER PZN-4.5%PT FERROELECTRIC SINGLE CRYSTAL
An extremely broad lower 2θ peak adjacent to the major (002) rhombohedral peak has been frequently observed in standard XRD profiles of bulk PZN-PT single crystals at room temperature. To understand the original and nature of this lower 2θ peak, high-resolution synchrotron X-ray diffraction study was carried out. The synchrotron (002) mapping together with a fracturing technique confirmed that the lower 2θ peak arises from a polishing-induced surface layer of "highly stressed rhombohedral state of monoclinic symmetry" which, structurally, may be likened to one full of "incipient monoclinic nuclei" of a range of lattice parameters. These "incipient" monoclinic nuclei/phases are microscopic in dimensions and are placed under intense in-plane compressive stress in the surface layer. All these contribute to the extreme broadness of the lower 2θ peak. The present work shows that deformation of relaxor single crystals occurs readily by stress-induced phase transformation of the material from the rhombohedral state to other lower symmetry states. The lower 2θ peak, and hence the "incipient" monoclinic surface layer, is fairly resistant to annealing and low-field poling but can be largely eliminated when the as-polished sample was poled to sufficiently high field (i.e., 1.5 kV/mm) at room temperature. After annealing, however, the "incipient" monoclinic surface layer became more resistant to poling such that remnant of the lower 2θ peak persisted even after high-field poling.
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