Cargando…

Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal

The detailed atomic structure of the binary icosahedral (i) ScZn(7.33) 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 Br...

Descripción completa

Detalles Bibliográficos
Autores principales: Yamada, Tsunetomo, Takakura, Hiroyuki, Euchner, Holger, Pay Gómez, Cesar, Bosak, Alexei, Fertey, Pierre, de Boissieu, Marc
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4937780/
https://www.ncbi.nlm.nih.gov/pubmed/27437112
http://dx.doi.org/10.1107/S2052252516007041
Descripción
Sumario:The detailed atomic structure of the binary icosahedral (i) ScZn(7.33) 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-YbCd(5.7) 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-ScZn(7.33) and i-YbCd(5.7) was found to lie in the icosahedron shell and the DFP where in i-ScZn(7.33) 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.