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Crystal structures of the relaxor oxide Pb2(ScTa)O6 in the paraelectric and ferroelectric states

机译:处于顺电和铁电状态的弛豫氧化物Pb2(ScTa)O6的晶体结构

摘要

The crystal structure of the relaxor ferroelectric Pb2ScTaO6 has been refined from high-resolution neutron time-of-flight powder diffraction data recorded at various temperatures from 4 to 400 K. Upon warming, Pb2ScTaO6 undergoes a first-order transition at 295 K from the rhombohedral ferroelectric state into the cubic paraelectric state. At 4.2 K, in the ferroelectric state, this compound adopts R3 space-group symmetry, with a = 8.15231 (7) Å and α = 89.8488 (3)°. At 400 K, in the paraelectric state, this compound adopts Fm3̄m space-group symmetry, with a = 8.15345 (3) Å. In the ferroelectric state, the Pb2+ coordination polyhedra are quite asymmetric, clearly indicating the presence of a stereoactive electron lone pair. The Sc3+ and Ta5+ ions are also shifted away from the centers of their respective octahedra, each toward an octahedral face. The large displacement parameters associated with both the Pb and the O ions, in the 400 K structure reveal significant local shifts of these ions from their ideal sites in the paraelectric state. Thus, the paraelectric to ferroelectric transition is driven by long-range cooperative ordering of the cation displacements. Synchrotron X-ray powder diffraction measurements are used to estimate the domain size of the Sc3+/Ta5+ ordering and the ferroelectric cation displacements as 88 nm and 10 nm, respectively.
机译:弛豫铁电体Pb2ScTaO6的晶体结构已从在4至400 K的各种温度下记录的高分辨率中子飞行时间粉末衍射数据中得到了完善。升温后,Pb2ScTaO6在距菱形面295 K处经历了一次转换。铁电态变为立方顺电态。在4.2 K时,在铁电状态下,该化合物采用R3空间群对称性,其中a = 8.15231(7)Å和α= 89.8488(3)°。在400 K下,处于顺电状态,该化合物采用Fm3̄m空间群对称性,其a = 8.15345(3)Å。在铁电状态下,Pb2 +配位多面体非常不对称,清楚地表明存在立体电子孤对。 Sc3 +和Ta5 +离子也从各自八面体的中心移开,每个离子都移向八面体面。在400 K结构中,与Pb和O离子相关的大位移参数揭示了这些离子在顺电状态下从其理想位置发生了明显的局部位移。因此,顺电向铁电的转变是由阳离子位移的长距离协同排序驱动的。同步加速器X射线粉末衍射测量用于估算Sc3 + / Ta5 +有序的畴尺寸和铁电阳离子位移分别为88 nm和10 nm。

著录项

  • 作者

    Woodward PM; Baba-Kishi KZ;

  • 作者单位
  • 年度 2002
  • 总页数
  • 原文格式 PDF
  • 正文语种 eng
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