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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...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
International Union of Crystallography
2016
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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 |
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author | Yamada, Tsunetomo Takakura, Hiroyuki Euchner, Holger Pay Gómez, Cesar Bosak, Alexei Fertey, Pierre de Boissieu, Marc |
author_facet | Yamada, Tsunetomo Takakura, Hiroyuki Euchner, Holger Pay Gómez, Cesar Bosak, Alexei Fertey, Pierre de Boissieu, Marc |
author_sort | Yamada, Tsunetomo |
collection | PubMed |
description | 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. |
format | Online Article Text |
id | pubmed-4937780 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | International Union of Crystallography |
record_format | MEDLINE/PubMed |
spelling | pubmed-49377802016-07-19 Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal Yamada, Tsunetomo Takakura, Hiroyuki Euchner, Holger Pay Gómez, Cesar Bosak, Alexei Fertey, Pierre de Boissieu, Marc IUCrJ Research Papers 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. International Union of Crystallography 2016-06-14 /pmc/articles/PMC4937780/ /pubmed/27437112 http://dx.doi.org/10.1107/S2052252516007041 Text en © Tsunetomo Yamada et al. 2016 http://creativecommons.org/licenses/by/2.0/uk/ This is an open-access article distributed under the terms of the Creative Commons Attribution Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited. |
spellingShingle | Research Papers Yamada, Tsunetomo Takakura, Hiroyuki Euchner, Holger Pay Gómez, Cesar Bosak, Alexei Fertey, Pierre de Boissieu, Marc Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title | Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title_full | Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title_fullStr | Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title_full_unstemmed | Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title_short | Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal |
title_sort | atomic structure and phason modes of the sc–zn icosahedral quasicrystal |
topic | Research Papers |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4937780/ https://www.ncbi.nlm.nih.gov/pubmed/27437112 http://dx.doi.org/10.1107/S2052252516007041 |
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