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. 2018 Jan 31;8:2025. doi: 10.1038/s41598-018-20470-6

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© The Author(s) 2018

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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(a) The intermediate scattering function Φ(Q, t) of (CuZr)₉₆Al₄ at a Q value of 0.7 Å⁻¹ at six measured temperatures. The solid lines are the fitting of the KWW function in the α-relaxation time range. (b) The dynamic susceptibility χ_T(t) of (CuZr)₉₆Al₄ at a Q value of 0.7 Å⁻¹ on a linear-log scale. (c) The four-point correlation function χ₄ for all types of atoms of (Cu₅₀Zr₅₀)Al₄ liquid. (d) A snapshot of (Cu₅₀Zr₅₀)Al₄ liquid at 923 K with mobility of grey atoms substantially slower than red atoms. To visible the mobilities of interior atoms, a sliced simulation box is shown.