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Sc-Zn 二十面体准晶的原子结构和准相位模式。

Atomic structure and phason modes of the Sc-Zn icosahedral quasicrystal.

机构信息

Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University , Miyagi 980-8577, Japan.

Division of Applied Physics, Faculty of Engineering, Hokkaido University , Hokkaido 060-8628, Japan.

出版信息

IUCrJ. 2016 Jun 14;3(Pt 4):247-58. doi: 10.1107/S2052252516007041. eCollection 2016 Jul 1.

Abstract

The detailed atomic structure of the binary icosahedral (i) ScZn7.33 quasicrystal has been investigated by means of high-resolution synchrotron single-crystal X-ray diffraction and absolute scale measurements of diffuse scattering. The average atomic structure has been solved using the measured Bragg intensity data based on a six-dimensional model that is isostructural to the i-YbCd5.7 one. The structure is described with a quasiperiodic packing of large Tsai-type rhombic triacontahedron clusters and double Friauf polyhedra (DFP), both resulting from a close-packing of a large (Sc) and a small (Zn) atom. The difference in chemical composition between i-ScZn7.33 and i-YbCd5.7 was found to lie in the icosahedron shell and the DFP where in i-ScZn7.33 chemical disorder occurs on the large atom sites, which induces a significant distortion to the structure units. The intensity in reciprocal space displays a substantial amount of diffuse scattering with anisotropic distribution, located around the strong Bragg peaks, that can be fully interpreted as resulting from phason fluctuations, with a ratio of the phason elastic constants K 2/K 1 = -0.53, i.e. close to a threefold instability limit. This induces a relatively large perpendicular (or phason) Debye-Waller factor, which explains the vanishing of 'high-Q perp' reflections.

摘要

采用高分辨率同步加速器单晶 X 射线衍射和漫散射的绝对标度测量,研究了二元二十面体(i)ScZn7.33 准晶的详细原子结构。基于与 i-YbCd5.7 相同的六维模型,利用测量的布拉格强度数据解决了平均原子结构。结构描述为大型 Tsai 型菱形三十面体簇和双 Friauf 多面体(DFP)的准周期堆积,两者均由大(Sc)和小(Zn)原子的紧密堆积产生。发现 i-ScZn7.33 和 i-YbCd5.7 之间的化学成分差异在于二十面体壳和 DFP 中,在 i-ScZn7.33 中,化学无序发生在大原子位置上,这导致结构单元发生显著变形。倒易空间中的强度显示出大量具有各向异性分布的漫散射,位于强布拉格峰周围,这些散射可完全解释为由位错涨落引起的,相位弹性常数 K2/K1 的比值为-0.53,即接近三倍不稳定性极限。这导致相对较大的垂直(或位错)德拜-沃勒因子,这解释了“高-Q 垂直”反射的消失。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eb64/4937780/2f56cbd74e5a/m-03-00247-fig1.jpg

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