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钡(1-x)锶(x)钛酸盐和钡钛(1-y)锆(y)氧体纳米晶的 X 射线吸收和 X 射线总散射研究。

Local structure of Ba(1-x)Sr(x)TiO3 and BaTi(1-y)Zr(y)O3 nanocrystals probed by X-ray absorption and X-ray total scattering.

机构信息

Department of Chemistry, University of Southern California , Los Angeles, California 90089, United States.

出版信息

ACS Nano. 2013 Dec 23;7(12):11435-44. doi: 10.1021/nn405629e. Epub 2013 Dec 2.

Abstract

The effect of isovalent chemical substitution on the magnitude and coherence length of local ferroelectric distortions present in sub-20 nm Ba(1-x)Sr(x)TiO3 (x = 0.0, 0.30, 0.50, 1.0) and BaTi(1-y)Zr(y)O3 (y = 0.0, 0.15, 0.50, 1.0) nanocrystals synthesized at room temperature is investigated using X-ray absorption near edge structure (XANES) and pair distribution function analysis of X-ray total scattering data (PDF). Although the average crystal structure of the nanocrystals is adequately described by a centrosymmetric, cubic Pm3m space group, local ferroelectric distortions due to the displacement of the titanium atom from the center of the perovskite lattice are observed for all compositions, except BaZrO3. The symmetry of the ferroelectric distortions is adequately described by a tetragonal P4mm space group. The magnitude of the local displacements of the titanium atom in BaTiO3 nanocrystals is comparable to that observed in single crystals and bulk ceramics, but the coherence length of their ferroelectric coupling is much shorter (≤20 Å). Substitution of Sr(2+) for Ba(2+) and of Zr(4+) for Ti(4+) induces a tetragonal-to-cubic transition of the room temperature local crystal structure, analogous to that observed for single crystals and bulk ceramics at similar compositions. This transition is driven by a reduction of the magnitude of the local displacements of the titanium atom and/or of the coherence length of their ferroelectric coupling. Replacing 50% of Ba(2+) with Sr(2+) slightly reduces the magnitude of the titanium displacement, but the coherence length is not affected. In contrast, replacing 15% of the ferroelectrically active Ti(4+) with Zr(4+) leads to a significant reduction of the coherence length. Deviations from the ideal solid solution behavior are observed in BaTi(1-y)Zr(y)O3 nanocrystals and are attributed to an inhomogeneous distribution of the barium atoms in the nanocrystal. Composition-structure relationships derived for Ba(1-x)Sr(x)TiO3 and BaTi(1-y)Zr(y)O3 nanocrystals demonstrate that the evolution of the room temperature local crystal structure with chemical composition parallels that of single crystals and bulk ceramics, and that chemical control over ferroelectric distortions is possible in the sub-20 nm size range. In addition, the potential of PDF analysis of total scattering data to probe compositional fluctuations in nanocrystals is demonstrated.

摘要

室温下合成的亚 20nm Ba(1-x)Sr(x)TiO3(x=0.0、0.30、0.50、1.0)和 BaTi(1-y)Zr(y)O3(y=0.0、0.15、0.50、1.0)纳米晶中同价化学取代对局部铁电畸变幅度和相干长度的影响,使用 X 射线吸收近边结构(XANES)和 X 射线总散射数据的配分函数分析(PDF)进行了研究。尽管纳米晶的平均晶体结构可以用中心对称的立方 Pm3m 空间群很好地描述,但除 BaZrO3 外,所有组成物中都观察到钛原子从钙钛矿晶格中心位移引起的局部铁电畸变。铁电畸变的对称性可以用四方 P4mm 空间群很好地描述。BaTiO3 纳米晶中钛原子的局部位移幅度与单晶和体陶瓷中观察到的幅度相当,但铁电耦合的相干长度要短得多(≤20Å)。Sr(2+)取代 Ba(2+)和 Zr(4+)取代 Ti(4+)诱导室温局部晶体结构从四方相到立方相的转变,类似于在相似组成的单晶和体陶瓷中观察到的转变。这种转变是由钛原子的局部位移幅度和/或铁电耦合的相干长度的减小驱动的。用 Sr(2+)取代 50%的 Ba(2+)会略微减小钛的位移幅度,但不会影响相干长度。相比之下,用 Zr(4+)取代 15%的铁电活性 Ti(4+)会导致相干长度显著减小。在 BaTi(1-y)Zr(y)O3 纳米晶中观察到偏离理想固溶行为的现象,这归因于纳米晶中钡原子的不均匀分布。Ba(1-x)Sr(x)TiO3 和 BaTi(1-y)Zr(y)O3 纳米晶的组成-结构关系表明,室温下局部晶体结构随化学成分的演变与单晶和体陶瓷的演变相似,并且在亚 20nm 尺寸范围内可以对铁电畸变进行化学控制。此外,还证明了 PDF 分析全散射数据探测纳米晶中组成波动的潜力。

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