Bi3n+1Ti7Fe3n–3O9n+11 Homologous Series: Slicing Perovskite Structure with Planar Interfaces Containing Anatase-like Chains
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文摘
The n = 3–6 members of a new perovskite-based homologous series Bi<sub>3n+1sub>Ti<sub>7sub>Fe<sub>3n–3sub>O<sub>9n+11sub> are reported. The crystal structure of the n = 3 Bi<sub>10sub>Ti<sub>7sub>Fe<sub>6sub>O<sub>38sub> member is refined using a combination of X-ray and neutron powder diffraction data (a = 11.8511(2) ?, b = 3.85076(4) ?, c = 33.0722(6) ?, S.G. Immm), unveiling the partially ordered distribution of Ti<sup>4+sup> and Fe<sup>3+sup> cations and indicating the presence of static random displacements of the Bi and O atoms. All Bi<sub>3n+1sub>Ti<sub>7sub>Fe<sub>3n–3sub>O<sub>9n+11sub> structures are composed of perovskite blocks separated by translational interfaces parallel to the (001)<sub>psub> perovskite planes. The thickness of the perovskite blocks increases with n, while the atomic arrangement at the interfaces remains the same. The interfaces comprise chains of double edge-sharing (Fe,Ti)O<sub>6sub> octahedra connected to the octahedra of the perovskite blocks by sharing edges and corners. This configuration shifts the adjacent perovskite blocks relative to each other over a vector <sup>1sup>/<sub>2sub>[110]<sub>psub> and creates S-shaped tunnels along the [010] direction. The tunnels accommodate double columns of the Bi<sup>3+sup> cations, which stabilize the interfaces owing to the stereochemical activity of their lone electron pairs. The Bi<sub>3n+1sub>Ti<sub>7sub>Fe<sub>3n–3sub>O<sub>9n+11sub> structures can be formally considered either as intergrowths of perovskite modules and polysynthetically twinned modules of the Bi<sub>2sub>Ti<sub>4sub>O<sub>11sub> structure or as intergrowths of the 2D perovskite and 1D anatase fragments. Transmission electron microscopy (TEM) on Bi<sub>10sub>Ti<sub>7sub>Fe<sub>6sub>O<sub>38sub> reveals that static atomic displacements of Bi and O inside the perovskite blocks are not completely random; they are cooperative, yet only short-range ordered. According to TEM, the interfaces can be laterally shifted with respect to each other over ±1/3a, introducing an additional degree of disorder. Bi<sub>10sub>Ti<sub>7sub>Fe<sub>6sub>O<sub>38sub> is paramagnetic in the 1.5–1000 K temperature range due to dilution of the magnetic Fe<sup>3+sup> cations with nonmagnetic Ti<sup>4+sup>. The n = 3, 4 compounds demonstrate a high dielectric constant of 70–165 at room temperature.

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