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Machine-learning-accelerated simulations to enable automatic surface reconstruction

A preprint version of the article is available at arXiv.

Abstract

Understanding material surfaces and interfaces is vital in applications such as catalysis or electronics. By combining energies from electronic structure with statistical mechanics, ab initio simulations can, in principle, predict the structure of material surfaces as a function of thermodynamic variables. However, accurate energy simulations are prohibitive when coupled to the vast phase space that must be statistically sampled. Here we present a bi-faceted computational loop to predict surface phase diagrams of multicomponent materials that accelerates both the energy scoring and statistical sampling methods. Fast, scalable and data-efficient machine learning interatomic potentials are trained on high-throughput density-functional-theory calculations through closed-loop active learning. Markov chain Monte Carlo sampling in the semigrand canonical ensemble is enabled by using virtual surface sites. The predicted surfaces for GaN(0001), Si(111) and SrTiO3(001) are in agreement with past work and indicate that the proposed strategy can model complex material surfaces and discover previously unreported surface terminations.

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Fig. 1: AutoSurfRecon framework.
Fig. 2: AL procedure for NFF.
Fig. 3: Obtaining the GaN(0001) contracted-monolayer surface reconstruction using VSSR-MC and a classical potential.
Fig. 4: AL for NFF.
Fig. 5: Analyzing dominant SrTiO3(001) surface terminations observed during VSSR-MC runs at different chemical potentials.
Fig. 6: Comparing DFT and NFF energies of double-layer TiO2 terminations, all with the same composition.

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Data availability

The trained models, DFT data and Jupyter notebooks used for data analysis are available on Zenodo at https://doi.org/10.5281/zenodo.7758174 (ref. 72). Source data are provided with this paper.

Code availability

The VSSR-MC algorithm reported in this work is available on GitHub at https://github.com/learningmatter-mit/surface-sampling. The version of code used in this work is available on Zenodo at https://doi.org/10.5281/zenodo.10086398 (ref. 73).

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Acknowledgements

We thank G. Winter, J. Peng, N. Frey and M. Liu for helpful discussions. We also appreciate editing by J. Peng and A. Hoffman. X.D. acknowledges support from the National Science Foundation Graduate Research Fellowship under grant no. 2141064. J.K.D. was supported by the Department of Defense through the National Defense Science and Engineering Graduate Fellowship Program. We are grateful for computation time allocated on the MIT SuperCloud cluster, the MIT Engaging cluster and the NERSC Perlmutter cluster. This material is based on work supported by the Under Secretary of Defense for Research and Engineering under Air Force Contract No. FA8702-15-D-0001. Any opinions, findings, conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the Under Secretary of Defense for Research and Engineering. Delivered to the US Government with Unlimited Rights, as defined in DFARS Part 252.227-7013 or 7014 (February 2014). Notwithstanding any copyright notice, US Government rights in this work are defined by DFARS 252.227-7013 or DFARS 252.227-7014 as detailed above. Use of this work other than as specifically authorized by the US Government may violate any copyrights that exist in this work.

Author information

Authors and Affiliations

Authors

Contributions

X.D. implemented the sampling algorithm, performed surface modeling, ran DFT calculations, trained the neural networks and carried out surface stability analysis. J.K.D. assisted with sampling algorithm implementation and provided guidance with surface modeling. J.R.L. provided guidance with surface modeling and ran DFT calculations. R.M. provided guidance with neural network training and active learning. B.Y. provided guidance with the choice of surfaces and surface stability analysis. L.L. supervised the research and contributed to securing funding. R.G.-B. conceived the project, supervised the research and contributed to securing funding. All authors contributed to results discussion and paper writing.

Corresponding author

Correspondence to Rafael Gómez-Bombarelli.

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Nature Computational Science thanks Mie Andersen and the other, anonymous, reviewer(s) for their contribution to the peer review of this work. Primary Handling Editor: Kaitlin McCardle, in collaboration with the Nature Computational Science team. Peer reviewer reports are available.

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Extended data

Extended Data Fig. 1 Top view of additional GaN(0001) MC-sampled structures.

The surface reconstructions are rotated in comparison with the reference structure from ref. 46 but contain the same hexagonal pattern.

Extended Data Fig. 2 Comparing classical potential and DFT energies of Si(111) sampled surface reconstructions.

ac, Structures shown were obtained from constant-composition (canonical) VSSR-MC sampling using the SRS modified Stillinger-Weber potential45 with 3x3 (a), 5x5 (b) and 7x7 (c) unit cells. The SRS energies were obtained from the depicted structures while the DFT energies came from structures further relaxed at the DFT level. * Further relaxation using DFT resulted in the 3x3 DAS structure.

Extended Data Fig. 3 Correlation plot of force MAE with force s.d. over AL generations.

At each AL generation, an ensemble of just three NFF models was able to estimate force s.d. that correlated strongly with force error. Each individual data point represents a sampled structure. Each blue ‘X’ represents a binned average and a best-fit line is drawn through the binned averages. The binned average is calculated by dividing both the force s.d. and force MAE into equal-sized bins. The average force MAE is then plotted against the median force s.d. for each corresponding bin.

Source data

Extended Data Fig. 4 Force distribution over AL generations.

The majority of high-force structures were added in AL generations 1, 2 and 6, which correspond either to random structures or structures obtained through adversarial attack. The three VSSR-MC AL generations produced structures with low force values mostly around 50 eV Å-1 or less.

Source data

Extended Data Fig. 5 Test performance of the best NFF model.

As described in the main paper, the test data is obtained from VSSR-MC runs using the sixth-generation NFF model.

Source data

Extended Data Fig. 6 Strengths and limitations of VSSR-MC.

a,b, Comparison of limited fixed on-lattice sites (a) and denser algorithmically-generated virtual surface sites that can overlap (b). c, Off-lattice reconstructions can be obtained following VSSR-MC discrete sampling at virtual sites and continuous relaxation of surface atoms and adsorbates. d, Amorphous reconstructions with many local minima, however, will likely be difficult for VSSR-MC to sample.

Extended Data Fig. 7 Side view of virtual sites for surfaces studied in this work.

ad, Pymatgen (a) and CatKit (b) virtual sites for GaN(0001) against the contracted Ga monolayer reconstruction, two-layer pymatgen sites for Si(111) against the 5x5 DAS reconstruction (c), and pymatgen virtual sites for SrTiO3(001) against the double-layer TiO2 reconstruction (d). The dashed lines are a guide for the eye.

Extended Data Fig. 8 Visualizations in the latent space.

a, Clustering of VSSR-MC structures in the NFF latent space visualized in the first three principal components. In the VSSR-MC with clustering AL method, the surface from each cluster with the highest force s.d. is selected for DFT evaluation. b, PCA of training data and the dominant terminations (term.) in the latent space of the sixth-generation model.

Source data

Supplementary information

Supplementary Information

Supplementary Sections: (1) abbreviations used; and (2) surface stability analysis.

Peer Review File

Supplementary Data 1

Comparison of AutoSurfRecon with existing computational methods for surface reconstruction. AutoSurfRecon automatically samples across many surface compositions and configurations while training an accurate NFF for low-cost energy prediction.

Source data

Source Data Fig. 3

Statistical source data: Typical GaN(0001) VSSR-MC run profile.

Source Data Fig. 4

Statistical source data: (b) force error and predicted force s.d. for the sixth-generation model; (c) latent space embedding PCA of surfaces acquired at each AL generation; (d) force and energy predictions of the model at each AL generation on the final test set.

Source Data Fig. 5

Statistical source data: (b) predicted surface free energies for each dominant termination across Sr and O chemical potentials; (c-e) predicted surface free energies of sampled structures at Sr chemical potentials of −10, −7 and −4 eV and O chemical potential of 0 eV.

Source Data Extended Data Fig. 3

Statistical source data: force error and predicted force s.d. over six AL generations.

Source Data Extended Data Fig. 4

Statistical source data: distribution of force magnitudes over six AL generations.

Source Data Extended Data Fig. 5

Statistical source data: predictions of the sixth-generation AL model on final test data.

Source Data Extended Data Fig. 8

Statistical source data: (a) PCA of test data in the latent space of the sixth-generation model; (b) PCA of the sixth-generation training data and dominant terminations in the latent space of the sixth-generation model.

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Du, X., Damewood, J.K., Lunger, J.R. et al. Machine-learning-accelerated simulations to enable automatic surface reconstruction. Nat Comput Sci 3, 1034–1044 (2023). https://doi.org/10.1038/s43588-023-00571-7

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