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    Generalizable machine-learned interatomic potential for all-inorganic halide double perovskites

    Zachary J. L. Bare1,*, Nima Karimitari1,*, John T. Barber1, Charles B. Musgrave2, and Christopher Sutton1,3,4,†

    • *These authors contributed equally to this work.
    • †Contact author: ca.sutton@utoronto.ca

    Phys. Rev. Materials 10, 055401 – Published 1 May, 2026

    DOI: https://doi.org/10.1103/n6dj-hlzm

    Abstract

    We present a fine-tuned machine learning interatomic potential (MLIP) for all inorganic halide perovskites (AA′BB′X6), which we use to investigate stability trends across 195 968 charge-balanced compositions. The MLIP accurately predicts the relative stability of cubic and distorted phases, capturing octahedral tilting effects that often favor lower-energy or nonperovskite ground states. For the entire set of examined materials, only 2% of compositions are metastable (ΔHd< 100 meV/atom) in the high-symmetry cubic phase. To rationalize this result, we analyze 23 730 CsA′BB′X6 compositions and show that stability in the cubic phase correlates with the size mismatch between A and A′ cations. Because the MLIP yields DFT-quality optimized structures, single-point DFT can be used efficiently to compute energies and band gaps. Assuming the cubic structure instead of the ground state structure, which typically contains various degrees of octahedral distortions, can lead to changes in the band-gap energy of up to 0.50 eV. The MLIP enables vibrational free-energy calculations via phonon density of states, allowing temperature-dependent phase stability predictions. These reveal several compounds that are predicted to transition from the (distorted) ground state phase (at T=0K) to high-symmetry cubic phases at elevated temperatures. Overall, this work provides a tool and dataset of DFT quality AA′BB′X6 structures for analyzing key structure−property relationships and supports the discovery of new perovskite compositions with more realistic stability and band-gap estimates than considering the cubic phase alone.

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