Abstract

Machine learning approaches have been successfully employed in many fields of computational chemistry and physics. However, atomistic simulations driven by machine-learned forces are still very challenging. Here we show that reactive self-sputtering from a beryllium surface can be simulated using neural network trained forces with an accuracy that rivals or exceeds other approaches. The key in machine learning from density functional theory calculations is a well-balanced and complete training set of energies and forces. We have implemented a refinement protocol that corrects the low extrapolation capabilities of neural networks by iteratively checking and improving the molecular dynamic simulations. The sputtering yield obtained for incident energies below 100 eV agrees perfectly with results from ab initio molecular dynamics simulations and compares well with earlier calculations based on pair potentials and bond-order potentials. This approach enables simulation times, sizes and statistics similar to what is accessible by conventional force fields and reaching beyond what is possible with direct ab initio molecular dynamics. We observed that a potential fitted to one surface, Be(0001), has to be augmented with training data for another surface, Be(011̄0), in order to be used for both.

Highlights

  • In molecular dynamics (MD) simulations energies and forces are complicated functions of nuclear coordinates and element types

  • With the purpose of testing the transferability of NNP5 to a different surface structure that had not been included in the training set, we performed self-sputtering simulations with an incident energy of 75 and 100 eV on a Be(0110) surface consisting of 480 atoms

  • The self-sputtering simulations based on the re ned neural network potential give promising results for small and large periodic cell-sizes of the Be(0001) surface

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Summary

Introduction

We can train the network on a nite set of energies and forces and its quality will depend very much on the choice and size of the training set and on the power of the global optimizer to reach a low-lying minimum. With the purpose of testing the transferability of NNP5 to a different surface structure that had not been included in the training set, we performed self-sputtering simulations with an incident energy of 75 and 100 eV on a Be(0110) surface consisting of 480 atoms. We obtained much smaller sputtering yields than reported by Ueda.[16] Applying an iterative re nement step as described above on Be(0110) and re tting the neural network, more reasonable results are obtained, albeit with a different potential (NNP6). The results of MD simulations by Ueda et al.[16] and Bjorkas et al.,[17] the data of Monte Carlo simulations (assuming a surface binding energy of 3.38 eV) by Roth et al.[21] and experimental results[22,23] are included for comparison

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