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Training machine-learning potentials for crystal structure prediction using disordered structures

Changho Hong, Jeong Min Choi, Wonseok Jeong, Sungwoo Kang, Suyeon Ju, Kyeongpung Lee, Jisu Jung, Yong Youn, and Seungwu Han
Phys. Rev. B 102, 224104 – Published 18 December 2020

Abstract

Prediction of the stable crystal structure for multinary (ternary or higher) compounds with unexplored compositions demands fast and accurate evaluation of free energies in exploring the vast configurational space. The machine-learning potential such as the neural network potential (NNP) is poised to meet this requirement but a dearth of information on the crystal structure poses a challenge in choosing training sets. Herein we propose constructing the training set from density functional theory (DFT)–based dynamical trajectories of liquid and quenched amorphous phases, which does not require any preceding information on material structures except for the chemical composition. To demonstrate suitability of the trained NNP in the crystal structure prediction, we compare NNP and DFT energies for Ba2AgSi3, Mg2SiO4, LiAlCl4, and InTe2O5F over experimental phases as well as low-energy crystal structures that are generated theoretically. For every material, we find strong correlations between DFT and NNP energies, ensuring that the NNPs can properly rank energies among low-energy crystalline structures. We also find that the evolutionary search using the NNPs can identify low-energy metastable phases more efficiently than the DFT-based approach. By proposing a way to developing reliable machine-learning potentials for the crystal structure prediction, this work paves the way to identifying unexplored multinary phases efficiently.

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  • Received 19 August 2020
  • Revised 2 November 2020
  • Accepted 2 December 2020

DOI:https://doi.org/10.1103/PhysRevB.102.224104

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Changho Hong1, Jeong Min Choi1, Wonseok Jeong1, Sungwoo Kang1, Suyeon Ju1, Kyeongpung Lee1, Jisu Jung1, Yong Youn2, and Seungwu Han1,*

  • 1Department of Materials Science and Engineering and Research Institute of Advanced Materials, Seoul National University, Seoul 08826, Korea
  • 2Center for Green Research on Energy and Environmental Materials and International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan

  • *hansw@snu.ac.kr

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Vol. 102, Iss. 22 — 1 December 2020

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Images

  • Figure 1
    Figure 1

    Unit cells of the stable phase of (a) Ba2AgSi3, (b) Mg2SiO4, (c) LiAlCl4, and (d) InTe2O5F.

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  • Figure 2
    Figure 2

    Correlation between DFT and NNP energies. Structures are fixed to metastable structures from USPEX (blue circles) or experimental structures from the ICSD that are relaxed by DFT (red squares). For both ΔEtotNNP and ΔEtotDFT, the reference energy is the DFT energy of the stable phase. Experimental structures are plotted as red squares. (a) Ba2AgSi3, (b) Mg2SiO4, (c) LiAlCl4, and (d) InTe2O5F.

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  • Figure 3
    Figure 3

    The distribution of G vectors in Ba2AgSi3 projected onto the first two principal-component axes (PC1 and PC2). The distribution of (a) Ba atoms, (b) Ag atoms, and (c) Si atoms. The projected density on each axis is plotted at the top and side.

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  • Figure 4
    Figure 4

    The lowest-energy structures of (a) Ba2AgSi3, (b) Mg2SiO4, (c) LiAlCl4, and (d) InTe2O5F found by USPEX in combination with NNP. (c) Same as Fig. 1.

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  • Figure 5
    Figure 5

    Δ EtotDFT vs ΔEtotNNP for Ba2AgSi3 with structures in Fig. 2 after augmentation of the training set with metastable structures from USPEX-NNP.

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