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.

Highlights

  • The network topology in disordered materials is an important structural descriptor for understanding the nature of disorder that is usually hidden in pairwise correlations

  • The most important feature in the diffraction data of a-SiO2 is that the first sharp diffraction peak (FSDP)[11,12,13,14] is observed in both X-ray and neutron diffraction data, whereas the second diffraction peak, the so-called principal peak (PP)[12,14], can be observed in only the neutron diffraction data because this peak reflects the packing of oxygen ­atoms[12,15], which is sensitive to neutrons

  • The FSDP was first discussed in 1­ 97616, it seems that the name “FSDP” was first used by Phillips in 1­ 98117

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Summary

Introduction

The network topology in disordered materials is an important structural descriptor for understanding the nature of disorder that is usually hidden in pairwise correlations. It was demonstrated that intermediate-range ordering arises from the periodicity of boundaries between successive cages in the network formed by the connection of regular ­SiO4 tetrahedra with shared oxygen atoms at the corners associated with the formation of a ring structure and a large c­ avity[21,22].

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