Buscaglia Vincenzo, Tripathi Saurabh, Petkov Valeri, Dapiaggi Monica, Deluca Marco, Gajović Andreja, Ren Yang
Institute for Energetics and Interphases, National Research Council (IENI-CNR), Via De Marini 6, I-16149 Genova, Italy.
J Phys Condens Matter. 2014 Feb 12;26(6):065901. doi: 10.1088/0953-8984/26/6/065901. Epub 2014 Jan 17.
High-resolution x-ray diffraction (XRD), Raman spectroscopy and total scattering XRD coupled to atomic pair distribution function (PDF) analysis studies of the atomic-scale structure of archetypal BaZrxTi(1-x)O3 (x = 0.10, 0.20, 0.40) ceramics are presented over a wide temperature range (100-450 K). For x = 0.1 and 0.2 the results reveal, well above the Curie temperature, the presence of Ti-rich polar clusters which are precursors of a long-range ferroelectric order observed below TC. Polar nanoregions (PNRs) and relaxor behaviour are observed over the whole temperature range for x = 0.4. Irrespective of ceramic composition, the polar clusters are due to locally correlated off-centre displacement of Zr/Ti cations compatible with local rhombohedral symmetry. Formation of Zr-rich clusters is indicated by Raman spectroscopy for all compositions. Considering the isovalent substitution of Ti with Zr in BaZrxTi1-xO3, the mechanism of formation and growth of the PNRs is not due to charge ordering and random fields, but rather to a reduction of the local strain promoted by the large difference in ion size between Zr(4+) and Ti(4+). As a result, non-polar or weakly polar Zr-rich clusters and polar Ti-rich clusters are randomly distributed in a paraelectric lattice and the long-range ferroelectric order is disrupted with increasing Zr concentration.
本文展示了对典型的BaZrₓTi₍₁₋ₓ₎O₃(x = 0.10、0.20、0.40)陶瓷在宽温度范围(100 - 450 K)内进行的高分辨率X射线衍射(XRD)、拉曼光谱以及与原子对分布函数(PDF)分析相结合的全散射XRD研究。对于x = 0.1和0.2,结果表明,在远高于居里温度时,存在富钛极性团簇,它们是在居里温度以下观察到的长程铁电有序的前驱体。对于x = 0.4,在整个温度范围内都观察到了极性纳米区域(PNR)和弛豫行为。无论陶瓷成分如何,极性团簇都是由于Zr/Ti阳离子的局域相关偏心位移,与局部菱面体对称性相兼容。拉曼光谱表明所有成分中都有富Zr团簇的形成。考虑到BaZrₓTi₁₋ₓO₃中Ti被Zr的等价取代,PNR的形成和生长机制不是由于电荷有序和随机场,而是由于Zr⁴⁺和Ti⁴⁺之间离子尺寸的巨大差异所促进的局部应变的降低。结果,非极性或弱极性的富Zr团簇和极性富钛团簇随机分布在顺电晶格中,并且随着Zr浓度的增加,长程铁电有序被破坏。