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abstracts
Recently, ferroelectricity was discovered in Sn-doped SrTiO3 (abbreviated by SSTO), in which Sr-atom was substituted by a few percent Sn-atom[1]. The ferroelctricity of SSTO was confirmed by means of the appearance of the dielectric anomaly, that reached several thousands and the clear D-E hysteresis loop in low temperature phase. In order to clarify the mechanism of ferroelectric phase transition of SSTO from the viewpoint of the crystal structure, we investigated the average crystal structure and the local structure around the substitutional Sn-atom of SSTO10 (10% Sn concentration, ferroelectric phase transition temperature 180K) by means of synchrotron-radiation powder X-ray diffraction and transmission XAFS spectrum of Sn:K-edge, respectively. From the results of MEM/Rietveld analysis of powder X-ray diffraction data, it was obtained that crystal structure of paraelectric phase of SSTO10 was cubic perovskite structure with the disorder state of Sn-atom. In ferroelectric phase, the crystal system was tetragonal, which was similar in structure to tetragonal ferroelectric structure of BaTiO3, and Sn-atom was order state. XAFS study revealed that the valence of Sn-ion was +2 charge and the local structure of Sn-atom was seemed as being the self-insistent state of SnO crystal structure. However, strangely, the coordination number of the nearest neighbor atom, that is O-atom, was 2 instead of 4. This is a mystery result and we have been analyzing. We have considered that the ferroelectricity of SSTO is induced by the distortion around the subsitituional Sn-atom. At the meeting, we are planning to discuss the precise crystal structure and the mechanism of the ferroelectric phase transition of SSTO.
abstracts
A great number of complicated intermetallic compounds were reported in binary and ternary alloy systems of Al with transition metals. Al–Co–Pd is one of the most interesting alloys, since a variety of crystalline phases associated with quasicrystals has been reported [1]. Among these crystalline phases, the structures of ε-phases are closely associated with Al3Pd, which is an important crystalline approximant for the decagonal phase with a period of 1.6 nm. W-phase is another approximant for the decagonal phase and its structural information is useful for understanding the columnar unit in the decagonal phase with a periodicity of 0.8 nm [2]. On the other hand, some crystalline phases associated with the icosahedral phase were also found in this Al-Pd-Co system. C2–phase, R-phase (R3: a = 2.91 nm, c = 1.32 nm) and F-phase (Pa3: a = 2.44 nm) are classified into this category. In particular, the structures of R-phase and F-phase consist of a variety of pseudo-Mackay clusters similar to those found in 1/1-AlCuRu and the trigonal χ-AlPdRe. As an example, the structure of R-phase shows two types of pMCs. These pMCs can be ranked by their atomic arrangements of the first shells, nevertheless every outer shell is a harmony of an Al-icosidodecahedron and a Co/Pd-icosahedron. These pMCs interpenetrate each other by sharing edges of Co/Pd-icosahedra and the interstitial space is subsequently filled by the smaller Al-icosahedra around Pd/Al sites [3]. The characteristic structural motifs for R-phase and F-phase readily suggest the importance of pMC as a fundamental structural unit for icosahedral quasicrystals.
