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Abstract
The network topology in disordered materials is an important structural descriptor for understanding the nature of disorder that is usually hidden in pairwise correlations. Here, we compare the covalent network topology of liquid and solidified silicon (Si) with that of silica (SiO2) on the basis of the analyses of the ring size and cavity distributions and tetrahedral order. We discover that the ring size distributions in amorphous (a)-Si are narrower and the cavity volume ratio is smaller than those in a-SiO2, which is a signature of poor amorphous-forming ability in a-Si. Moreover, a significant difference is found between the liquid topology of Si and that of SiO2. These topological features, which are reflected in diffraction patterns, explain why silica is an amorphous former, whereas it is impossible to prepare bulk a-Si. We conclude that the tetrahedral corner-sharing network of AX2, in which A is a fourfold cation and X is a twofold anion, as indicated by the first sharp diffraction peak, is an important motif for the amorphous-forming ability that can rule out a-Si as an amorphous former. This concept is consistent with the fact that an elemental material cannot form a bulk amorphous phase using melt quenching technique.
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Details
1 National Institute for Materials Science, Research Center for Advanced Measurement and Characterization, Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880); ETH Zürich, Department of Earth Science, Zürich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780)
2 Gifu University, Department of Electrical, Electronic and Computer Engineering, Faculty of Engineering, Gifu, Japan (GRID:grid.256342.4) (ISNI:0000 0004 0370 4927); RIKEN, Center for Advanced Intelligence Project, Tokyo, Japan (GRID:grid.7597.c) (ISNI:0000000094465255)
3 National Institute for Materials Science, Research Center for Advanced Measurement and Characterization, Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880); Kyoto University, Institute for Integrated Radiation and Nuclear Science, Osaka, Japan (GRID:grid.258799.8) (ISNI:0000 0004 0372 2033)
4 National Institute of Advanced Industrial Science and Technology (AIST), Department of Materials and Chemistry, Ikeda, Japan (GRID:grid.208504.b) (ISNI:0000 0001 2230 7538)
5 Waseda University, Department of Materials Science, Shinjuku, Japan (GRID:grid.5290.e) (ISNI:0000 0004 1936 9975); Waseda University, Kagami Memorial Research Institute for Materials Science and Technology, Shinjuku, Japan (GRID:grid.5290.e) (ISNI:0000 0004 1936 9975); Tohoku University, Mathematics for Advanced Materials Open Innovation Laboratory (MathAM-OIL), AIST, c/o AIMR, Sendai, Japan (GRID:grid.69566.3a) (ISNI:0000 0001 2248 6943)
6 ETH Zürich, Department of Earth Science, Zürich, Switzerland (GRID:grid.5801.c) (ISNI:0000 0001 2156 2780)
7 Tohoku University, Mathematics for Advanced Materials Open Innovation Laboratory (MathAM-OIL), AIST, c/o AIMR, Sendai, Japan (GRID:grid.69566.3a) (ISNI:0000 0001 2248 6943); AIST, Research Center for Computational Design of Advanced Functional Materials (CD-FMat), Tsukuba, Japan (GRID:grid.208504.b) (ISNI:0000 0001 2230 7538)
8 Nagoya Institute of Technology, Department of Physical Science and Engineering, Nagoya, Japan (GRID:grid.47716.33) (ISNI:0000 0001 0656 7591)
9 Nagoya Institute of Technology, Department of Physical Science and Engineering, Nagoya, Japan (GRID:grid.47716.33) (ISNI:0000 0001 0656 7591); Nagoya Institute of Technology, Frontier Research Institute for Materials Research, Nagoya, Japan (GRID:grid.47716.33) (ISNI:0000 0001 0656 7591)