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Structure solution of the basic decagonal Al-Co-Ni phase by the atomic surfaces modelling method [Review]

机译:基本十角形Al-Co-Ni相结构的原子表面建模方法[综述]

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The atomic surfaces modelling technique has been used to solve the structure of the basic Ni-rich Al-Co-Ni decagonal phase. Formula Al70.6Co6.7Ni22.7, space group P (10) over bar, five-dimensional unit-cell parameters: d(1) = d(4) = 4.752 (3) Angstrom, d(2) = d(3) = 3.360 (2) Angstrom, d(5) = 8.1710 (2) Angstrom; alpha(12) = alpha(34) = 69.295degrees, alpha(13) = alpha(24) = 45degrees, alpha(14) = 41.410degrees, alpha(23) = alpha(i5) = 90degrees (i = 1-4), V = 291.2 (7) Angstrom(5); D-x = 3.887 Mg m(-3). Refinement based on F ; 2767 unique reflections ( F > 0), 749 parameters, R = 0.17, wR = 0.06. Describing the structure of quasicrystals embedded in n-dimensional superspace in principle takes advantage of n-dimensional periodicity to select the minimal set of degrees of freedom for the structure. The method of modelling of the atomic surfaces yielded the first fully detailed structure solution of this phase. Comparison with numerous former, less accurate models confirms several features already derived, but adds a new essential insight of the structure and its complexity. The atoms fill the space forming recurrent structure motifs, which we will (generically) refer to as clusters. However, no unique cluster exists, although differences are small. Each cluster shows a high degree of structural disorder. This gives rise to a large configurational entropy, as much as expected in a phase which is stable at high temperature. On the other side, the cluster spatial arrangement is perfectly quasiperiodic. These considerations, corroborated by analysis of the structural relationship with neighbouring periodic phases, strongly suggest the existence of a non-local, long-range interaction term in the total energy which may be essential to the stability. [References: 182]
机译:原子表面建模技术已用于解决基本富镍Al-Co-Ni十方相的结构。公式Al70.6Co6.7Ni22.7,空间组P(10)超过条形,五维晶胞参数:d(1)= d(4)= 4.752(3)埃,d(2)= d(3 )= 3.360(2)埃,d(5)= 8.1710(2)埃; alpha(12)= alpha(34)= 69.295度,alpha(13)= alpha(24)= 45度,alpha(14)= 41.410度,alpha(23)= alpha(i5)= 90度(i = 1-4 ),V = 291.2(7)埃(5); D-x = 3.887Mg·m(-3)。基于F的细化; 2767次唯一反射(F> 0),749个参数,R = 0.17,wR = 0.06。原则上描述嵌入n维超空间中的准晶体的结构是利用n维周期性来选择结构的最小自由度集。原子表面建模的方法得出了该阶段的第一个完整的详细结构解决方案。与众多以前不太准确的模型进行比较,证实了已经得出的几个特征,但是增加了对结构及其复杂性的新的基本认识。原子填充形成循环结构图案的空间,我们将其(通常)称为簇。但是,尽管差异很小,但不存在唯一的群集。每个簇显示高度的结构紊乱。这引起了大的结构熵,正如在高温下稳定的相中所期望的那样。另一方面,簇的空间布置是完全准周期的。这些考虑通过分析与相邻周期相的结构关系得到了证实,有力地表明总能量中存在一个非局部的,长程相互作用项,这可能对稳定性至关重要。 [参考:182]

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