Recent application of neural networks (NNs) to modeling interatomic interactions has shown the learning machines' encouragingly accurate performance for select elemental and multicomponent systems. In this study, we explore the possibility of building a library of NN-based models by introducing a hierarchical NN training. In such a stratified procedure NNs for multicomponent systems are obtained by sequential training from the bottom up: first unaries, then binaries, and so on. Advantages of constructing NN sets with shared parameters include acceleration of the training process and intact description of the constituent systems. We use an automated generation of diverse structure sets for NN training on density functional theory-level reference energies. In the test case of Cu, Pd, Ag, Cu-Pd, Cu-Ag, Pd-Ag, and Cu-Pd-Ag systems, NNs trained in the traditional and stratified fashions are found to have essentially identical accuracy for defect energies, phonon dispersions, formation energies, etc. The models' robustness is further illustrated via unconstrained evolutionary structure searches in which the NN is used for the local optimization of crystal unit cells.
Prescreening candidate structures with reliable classical
potentials
is an effective way to accelerate ab initio ground
state searches. Given the growing popularity of machine learning force
fields, surprisingly little work has been dedicated to quantifying
their advantages over traditional potentials in global structure optimizations.
In this study, we have developed a neural network (NN) model and systematically
benchmarked it against a commonly used Gupta potential and an embedded
atom model in the search for stable Au
N
clusters (30 ≤ N ≤ 80). An efficient
simultaneous optimization of clusters in the full size range was achieved
with our recently introduced multitribe evolutionary algorithm. Density
functional theory (DFT) evaluations of candidate configurations identified
with the three classical models revealed that the NN structures were
lower in energy by at least 10 meV/atom for 30 of the 51 sizes. We
also demonstrated that DFT evaluation of all NN-relaxed structures during evolutionary searches resulted in finding even more
stable configurations, which highlights the need for further improvement
of the NN accuracy to avoid excessive DFT calculations. Overall, the
global searches produced putative ground states with matching or lower
DFT energies compared to all previously reported Au clusters with
30–80 atoms.
We have discovered a stoichiometric LiB with hexagonal boron layers by compressing known LiB0.9 with linear boron chains. The sp to sp 2 rebonding occurred at room temperature and moderate pressures above 21 GPa. The study was motivated by a long-standing prediction that LiB in the stable layered configuration could be a close analog to the MgB2 superconductor. Apparent stacking disorder in LiB and an evidenced stoichiometry shift in LiBy (down to y ≈ 0.75) made the materials' characterization a challenge. Ab initio modeling allowed us to establish LiBy's pressure-dependent composition and predict overlooked related stable structures. The synchrotron powder diffraction data indicates that synthesized LiB remains metastable under ambient pressure.
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