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BIGDML-Towards accurate quantum machine learning force fields for materialsopen access

Authors
Sauceda, Huziel E.Galvez-Gonzalez, Luis E.Chmiela, StefanOliver Paz-Borbon, LauroMueller, Klaus-RobertTkatchenko, Alexandre
Issue Date
29-Jun-2022
Publisher
NATURE PORTFOLIO
Citation
NATURE COMMUNICATIONS, v.13, no.1
Indexed
SCIE
SCOPUS
Journal Title
NATURE COMMUNICATIONS
Volume
13
Number
1
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/143881
DOI
10.1038/s41467-022-31093-x
ISSN
2041-1723
Abstract
Most machine-learning force fields dismiss long-range interactions. Here the authors demonstrate the BIGDML approach for building materials' potential energy surfaces that enables a broad range of materials simulations within accuracies better than 1 meV/atom using just 10-200 structures for training. Machine-learning force fields (MLFF) should be accurate, computationally and data efficient, and applicable to molecules, materials, and interfaces thereof. Currently, MLFFs often introduce tradeoffs that restrict their practical applicability to small subsets of chemical space or require exhaustive datasets for training. Here, we introduce the Bravais-Inspired Gradient-Domain Machine Learning (BIGDML) approach and demonstrate its ability to construct reliable force fields using a training set with just 10-200 geometries for materials including pristine and defect-containing 2D and 3D semiconductors and metals, as well as chemisorbed and physisorbed atomic and molecular adsorbates on surfaces. The BIGDML model employs the full relevant symmetry group for a given material, does not assume artificial atom types or localization of atomic interactions and exhibits high data efficiency and state-of-the-art energy accuracies (errors substantially below 1 meV per atom) for an extended set of materials. Extensive path-integral molecular dynamics carried out with BIGDML models demonstrate the counterintuitive localization of benzene-graphene dynamics induced by nuclear quantum effects and their strong contributions to the hydrogen diffusion coefficient in a Pd crystal for a wide range of temperatures.
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