TY - JOUR
T1 - Relationship between diffraction peak, network topology, and amorphous-forming ability in silicon and silica
AU - Kohara, Shinji
AU - Shiga, Motoki
AU - Onodera, Yohei
AU - Masai, Hirokazu
AU - Hirata, Akihiko
AU - Murakami, Motohiko
AU - Morishita, Tetsuya
AU - Kimura, Koji
AU - Hayashi, Kouichi
N1 - Funding Information:
This research was supported by the TIA collabo rative research program "Kakehashi", Grant Number TK19-004 (to S.K. and H.M.), and JSPS KAKENHI Grant Numbers 20H05878 (to M.S., S.K., and K.H.), 20H05881 (to S.K., Y.O., A.H., and K.K.), 20H05884 (to M.S.), 20H04241 (to S.K., M.S., Y.O., and A.H.), 19K05648 (to Y.O.), and 19K22072 (to S.K., Y.O, and H.M.). Discussion with László Pusztai is gratefully appreciated.
Publisher Copyright:
© 2021, The Author(s).
PY - 2021/12
Y1 - 2021/12
N2 - 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.
AB - 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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U2 - 10.1038/s41598-021-00965-5
DO - 10.1038/s41598-021-00965-5
M3 - Article
C2 - 34772967
AN - SCOPUS:85118953935
VL - 11
JO - Scientific Reports
JF - Scientific Reports
SN - 2045-2322
IS - 1
M1 - 22180
ER -