Displacive Order–Disorder Behavior and Intrinsic Clustering of Lattice Distortions in Bi‐Substituted NaNbO3

材料科学 八面体 格子(音乐) 凝聚态物理 自然键轨道 结晶学 纳米尺度 固溶体 钙钛矿(结构) 化学物理 晶体结构 密度泛函理论 纳米技术 物理 计算化学 化学 声学 冶金
作者
Igor Levin,Fan Yang,Russell A. Maier,W. Laws,Dean S. Keeble,Giannantonio Cibin,Derek C. Sinclair
出处
期刊:Advanced Functional Materials [Wiley]
卷期号:30 (30) 被引量:21
标识
DOI:10.1002/adfm.202001840
摘要

Abstract Perovskite‐like NaNbO 3 ‐Bi 1/3 NbO 3 solid solutions are studied to understand the interactions between octahedral rotations, which dominate the structural behavior of NaNbO 3 and displacive disorder of Bi present in Bi 1/3 NbO 3 . Models of instantaneous structures for representative compositions are obtained by refining atomic coordinates against X‐ray total scattering and extended X‐ray‐absorption fine structure data, with additional input obtained from transmission electron microscopy. A mixture of distinct cations and vacancies on the cuboctahedral A‐sites in Na 1−3 x Bi x NbO 3 ( x ≤ 0.2) results in 3D nanoscale modulations of structural distortions. This phenomenon is determined by the inevitable correlations in the chemical composition of adjacent unit cells according to the structure type—an intrinsic property of any nonmolecular crystals. Octahedral rotations become suppressed as x increases. Out‐of‐phase rotations vanish for x > 0.1, whereas in‐phase tilts persist up to x = 0.2, although for this composition their correlation length becomes limited to the nanoscale. The loss of out‐of‐phase tilting is accompanied by qualitative changes in the probability density distributions for Bi and Nb, with both species becoming disordered over loci offset from the centers of their respective oxygen cages. Symmetry arguments are used to attribute this effect to different strengths of the coupling between the cation displacements and out‐of‐phase versus in‐phase rotations. The displacive disorder of Bi and Nb combined with nanoscale clustering of lattice distortions are primarily responsible for the anomalous broadening of the temperature dependence of the dielectric constant.

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