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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Yamada, Tsunetomo
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Publications (5/5 displayed)
- 2020Growth and characterisation of single grain Al-Cu-Ru icosahedral quasicrystals from self-fluxescitations
- 2017Atomic structures of the Sc-Zn and R-Cd icosahedral quasicrystals
- 201745Sc and 67Zn NMR studies in Tsai-type quasicrystal and approximant.
- 2017Atomic structures of ternary Yb–Cd–Mg icosahedral quasicrystals and a 1/1 approximantcitations
- 2016Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystalcitations
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article
Atomic structure and phason modes of the Sc–Zn icosahedral quasicrystal
Abstract
<jats:p>The detailed atomic structure of the binary icosahedral (i) ScZn<jats:sub>7.33</jats:sub>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<jats:sub>5.7</jats:sub>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<jats:sub>7.33</jats:sub>and i-YbCd<jats:sub>5.7</jats:sub>was found to lie in the icosahedron shell and the DFP where in i-ScZn<jats:sub>7.33</jats:sub>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<jats:italic>K</jats:italic><jats:sub>2</jats:sub>/<jats:italic>K</jats:italic><jats:sub>1</jats:sub>= −0.53,<jats:italic>i.e.</jats:italic>close to a threefold instability limit. This induces a relatively large perpendicular (or phason) Debye–Waller factor, which explains the vanishing of `high-<jats:italic>Q</jats:italic><jats:sub>perp</jats:sub>' reflections.</jats:p>