Journal
JOURNAL OF NON-CRYSTALLINE SOLIDS
Volume 625, Issue -, Pages -Publisher
ELSEVIER
DOI: 10.1016/j.jnoncrysol.2023.122714
Keywords
Multi-component glass; First-principles calculations; Large-scale DFT; Classical force fields; Molecular dynamics simulations
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Although molecular dynamics (MD) simulation is a powerful tool for investigating the atomic-scale structures of complex materials, its reliable and accurate application to multi-component glass systems faces challenges due to limited force fields (FFs) and the complexity of chemical environments. This study demonstrates the feasibility of efficient and accurate large-scale density functional theory (DFT) calculations for multi-component glass systems. The evaluation of classical FFs based on the results of large-scale DFT calculations reveals low accuracy for non-bridging oxygen atoms, and differences in Si-O-Si angle distribution and electronic structure for X = Mg.
Although molecular dynamics (MD) simulation is a powerful tool for investigating the atomic-scale structures of complex materials, several challenges limit their reliable and accurate application to multi-component glass systems. The available force fields (FFs) that can treat many elements in a multi-component glass are limited, and even if such a FF exists, its accuracy is suspicious due to the large variety and complexity of chemical environments in these materials. First-principles calculations based on the density functional theory (DFT) are reliable, but prohibitively expensive with conventional methods. In this study, we use large-scale DFT techniques and demonstrate that it is possible to perform efficient and accurate DFT calculations of multi-component glass systems, such as (SiO2)0.70(Al2O3)0.13(XO)0.17 (X = Mg, Ca, Sr, Ba), containing about 1000-5000 atoms. From the results of large-scale DFT calculations, we evaluate the accuracy of some classical FFs, and show that the accuracy for non-bridging oxygen atoms is very low especially when the Si-O distance is short. Large differences in the distribution of Si-O-Si angles observed in the FF-MD and DFT-MD simulations and the unique electronic structure in the case of X = Mg are also discussed.
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