Abstract
Conduction of protons in solids is a cooperative process propelled by phonons, with molecular details obscured by the irregular movements in the thermal bath. We show that substitution with Y forms an imaginary phonon mode, instrumental for the function as proton conductor and effectively lowering the activation barrier for proton transport. To untangle the interplay in the exemplary proton conductor BaSn0.9Y0.1O3, we determine its crystallographic structure with high resolution neutron diffractometry and its phonon density of states with density functional theory calculations, experimentally validated by element specific nuclear resonant vibration spectroscopy. Based on phonon analysis, we present a quantitative transport model which predicts the activation energy and performance by the ratio of ionic radii. Rather than individual vibrational modes, it is the oxygen sub-lattice which exerts its momentum on the protons. The extent of this momentum transfer is governed by the ratio of ionic radii. Our model extends the transition state theory by the phonon-phonon interaction and complements the previously proposed idea that lattice dynamics is decisive for proton transport and specifies which properties of the material exactly define the vibration properties.
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Github repository with the scripts implementing the calculations, described in the manuscript
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TS.ipynb in test branch is the code that was used for the calculations
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Configuration generator for MatterSime fine-tune with QE
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Set of scripts used for genertion, post-processing and analysis of configurations for fine-tuning MatterSim model with QuantumEspresso DFT calculation.
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MatterSim fine-tuned MLIP for BaSnO₃ and Y-doped BaSnO₃ perovskites with oxygen vacancies
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The checkpoint of a fine-tuned MatterSim MLIP [https://doi.org/10.48550/arXiv.2405.04967] based on the pretrained model MatterSim-v1.0.0-5M. The potential was trained on the DFT calculations performed in Quantum Espresso. The training set consisted of the configurations including BaSnO3 and BaSn1-xYxO3 with perovskite structure.
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