name: cemdi-paims-jul26 class: title, middle, hide-slide-number ### Comparing MLIPs vs DFT for ionic conductivity in solid lithium electrolytes .bigger[Work led by Dounia Shaaban Kabakibo] Alex Hernández-García (presenting) .turquoise[[4th CEMDI–PAIMS Symposium 2026](https://cemdi.ca//symposium.php?id=evt_4th_symposium_2026) · Montréal · July 31st 2026] .center[
    
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] .smaller[.footer[ Slides: [alexhernandezgarcia.com/slides/{{ name }}](https://alexhernandezgarcia.com/slides/{{ name }}) ]] .qrcode[] --- count: false name: solid-state-electrolytes class: title, middle ## Design of novel lithium electrolytes with high ionic conductivity for solid-state batteries .center[
.smaller[Adapted from:
Murata
]
] --- class: hide-slide-number ## Traditional screening .center[
.smaller[Source:
He et al. (2020)
]
] .references[He et al. [High-throughput screening platform for solid electrolytes combining hierarchical ion-transport prediction algorithms](https://www.nature.com/articles/s41597-020-0474-y). Scientific Data, 2020.] --- class: hide-slide-number ## Screening guided by machine learning .center[
.smaller[Source:
Sendek et al. (2018)
]
] .references[Sendek et al. [Machine learning-assisted discovery of solid Li-ion conducting materials](https://pubs.acs.org/cmatex/article-abstract/31/2/342/1287786/Machine-Learning-Assisted-Discovery-of-Solid-Li). Chemistry of Materials, 2018.] --- ## Our approach ### Iterative _de novo_ design with generative models and active learning .right-column-66[.center[]] .left-column-33[ .highlight2[Iterative active learning]: * mimics the .h1[traditional scientific discovery cycle], * enables .h1[continuous improvement and refinement]. ] -- .left-column-33[ .highlight2[Generative machine learning] can: * .highlight1[explore] unseen regions of the search space and * propose .highlight1[novel candidates _de novo_]. ] --- ## _Multi-fidelity_ active learning with generative modelling .right-column-66[
.center[]] .left-column-33[
.highlight1[Multi-fidelity active learning] can: * leverage the availability of .highlight1[multiple oracles] with different .highlight1[costs and fidelity] * efficiently use the right level of accuracy needed for each query ] .references[Hernandez-Garcia, Saxena et al. [Multi-fidelity active learning with GFlowNets](https://arxiv.org/abs/2306.11715). TMLR, 2024] --- count: false ## _Multi-fidelity_ active learning with generative modelling .right-column-66[
.center[]] .left-column-33[
.highlight1[Multi-fidelity active learning] can: * leverage the availability of .highlight1[multiple oracles] with different .highlight1[costs and fidelity] * efficiently use the right level of accuracy needed for each query .conclusion-float[Multi-fidelity active learning can leverage the diversity of methods available in science.] ] .references[Hernandez-Garcia, Saxena et al. [Multi-fidelity active learning with GFlowNets](https://arxiv.org/abs/2306.11715). TMLR, 2024] --- count: false name: solid-state-electrolytes class: title, middle ## Design of novel lithium electrolytes with high ionic conductivity for solid-state batteries .center[
.smaller[Adapted from:
Murata
]
] --- ## Generative model ### Crystal-GFN .context[Presented at the 2nd CEMDI Symposium in 2024.] .right-column[.center[]] .left-column[ .h1[Generative ML model]: - The generated candidates should: - have the target property - have other desirable properties (lithium, available elements, etc.) - be realistic (physical constraints) - be diverse - The available data sets are extremely small for ML standards. ] --- ## Crystal-GFlowNet .center[] .conclusion-float[Crystal-GFN is a sequential generative model of crystal structures, to design candidates with desirable properties and constraints and inspired by theoretical crystallography.] .references[Mila AI4Science et al. [Crystal-GFN: sampling crystals with desirable properties and constraints](https://arxiv.org/abs/2310.04925). AI4Mat, NeurIPS 2023 (spotlight)] --- ## Data ### OBELiX .context[Presented at the 3rd CEMDI Symposium in 2025.] .right-column-66[.center[]] .left-column-33[ .h1[Data]: * Scarce and scattered data * Especially of high quality * Not ready for ML use ] --- ## OBELiX ### Open solid Battery Electrolytes with Li: an eXperimental dataset
.right-column-66[.center[]] .left-column-33[ We curated a data set of nearly 600 materials with experimentally measured ionic conductivity.
.center[] ] .full-width[ - Paper: [arxiv.org/abs/2502.14234](https://arxiv.org/abs/2502.14234) - Code and data set: [github.com/NRC-Mila/OBELiX](https://github.com/NRC-Mila/OBELiX/tree/main) ] --- ## OBELiX ### Open solid Battery Electrolytes with Li: an eXperimental dataset .center[] - Ionic conducitivities at room temperature - Composition, space groups and lattice parameters for all 599 materials - CIF files (structure) for 321 materials - Strict train, validation, test splits to avoid data leakage .references[ - Paper: [arxiv.org/abs/2502.14234](https://arxiv.org/abs/2502.14234) - Code and data set: [github.com/NRC-Mila/OBELiX](https://github.com/NRC-Mila/OBELiX/tree/main) ] --- ## ML predictive model .context[Presented at the 3rd CEMDI Symposium in 2025.] .right-column[.center[]] .left-column[ .h1[ML predictive model]: - Random forest - Multi-layer perceptron - Graph neural networks - ... ] --- count: false ## ML predictive model .context[Presented at the 3rd CEMDI Symposium in 2025.] .right-column[.center[]] .left-column[ .h1[ML predictive model]: - Random forest - Multi-layer perceptron - Graph neural networks - ...
.center[] ] --- count: false ## Oracle .context[Today, the 4th CEMDI Symposium in 2026.] .right-column-66[.center[]] .left-column-33[ .h1[Oracle]: experimental validation - Requires synthesising the material - Very high financial cost and multiple months per candidate. ] --- ## Oracle.h1[s] .context[Today, the 4th CEMDI Symposium in 2026.] .right-column-66[.center[]] .left-column-33[ .h1[Oracles]: - Experimental validation - .h2[DFT] - .h2[MLIPs] - ... ] --- ## Oracle.h1[s] .context[Today, the 4th CEMDI Symposium in 2026.] .right-column-66[.center[]] .left-column-33[ .h1[Oracles]: - Experimental validation - .h2[DFT] - .h2[MLIPs] - ... .conclusion-float[What is the accuracy and the cost of DFT and MLIPs to estimate the ionic conductivity?] ] --- ## Ionic conductivity estimation ### A comparison of methods .context[DFT has been widely used to estimate the ionic conductivity and recently MLIPs are widely available too.] .left-column-33[.center[] Paper: [arxiv.org/abs/2603.28012](https://arxiv.org/abs/2603.28012) ] .right-column-66[.center[]] --- ## Methodology - .h1[Goal]: Benchmark molecular dynamics (MD) approaches to estimate the ionic conductivity of lithium solid-state electrolytes. -- - A guiding objective was to also establish a framework that enables systematic comparisons across additional calculators and materials. -- - .h1[MD methods]: - DFT - MLIPs: NequIP, MACE and CHGNet -- - .h1[Data]: 76 lithium solid-state electrolytes from [OBELiX data set](https://pubs.rsc.org/en/content/articlepdf/2026/dd/d5dd00441a), with experimentally measured ionic conductivity. -- - Structures without disorder - DFT was evaluated on a subset of 21 structures. --- ## Ionic conductivity estimation .left-column[ For each material and method: ] --- count: false ## Ionic conductivity estimation .left-column[ For each material and method: 1. 100 ps MD at 5 temperatures: 800, 900, 1000, 1100 and 1200 K. ] .right-column[ .center[] ] --- count: false ## Ionic conductivity estimation .left-column[ For each material and method: 1. 100 ps MD at 5 temperatures: 800, 900, 1000, 1100 and 1200 K. 2. Obtain the slope $D$ of the mean square displacement of Li over time. ] .right-column[ .center[] ] --- count: false ## Ionic conductivity estimation .left-column[ For each material and method: 1. 100 ps MD at 5 temperatures: 800, 900, 1000, 1100 and 1200 K. 2. Obtain the slope $D$ of the mean square displacement of Li over time. 3. Extrapolate to room temperature via Arrhenius. ] .right-column[ .center[] .center[] ] --- count: false ## Ionic conductivity estimation .left-column[ For each material and method: 1. 100 ps MD at 5 temperatures: 800, 900, 1000, 1100 and 1200 K. 2. Obtain the slope $D$ of the mean square displacement of Li over time. 3. Extrapolate to room temperature via Arrhenius. 4. Estimate the ionic conductivity $\sigma$ via the Nernst-Einstein relation. ] .right-column[ .center[] .center[] ] --- ## Results #### NequIP vs DFT vs experimental .full-width[.center[]] --- count: false ## Results #### NequIP vs DFT vs experimental .full-width[.center[]] --- count: false ## Results #### NequIP vs DFT vs experimental .full-width[.center[]] --- count: false ## Results #### NequIP vs DFT vs experimental .full-width[.center[]] .conclusion[The DFT-estimated ionic conductivities exhibit weak correlation with experimental measurements (bad news), but the correlation of the MLIP-based estimations is only slightly weaker (good news).] --- ## Results: all vs. all .left-column-66[.center[]] -- .right-column-33[ .conclusion-float[NequIP correlates best with DFT, then MACE, then CHGNet.] ] -- .right-column-33[ .conclusion-float[NequIP and MACE are well correlated, more than with CHGNet.] ] --- ## Results ### Estimation time We measure the wall time to estimate to ionic conductivity of each material with every method. .center[] .conclusion[DFT needs disproportionally more time than MLIPs; NequIP still needs about 3 hours per material, significantly longer than MACE.] --- ## Summary - .h1[Crystal-GFN] offers a flexible framework for crystal structure generation with desirable properties and constraints, based on sequential decision making. - Mila AI4Science et al. [Crystal-GFN: sampling crystals with desirable properties and constraints](https://arxiv.org/abs/2310.04925). AI4Mat, NeurIPS 2023 (spotlight). -- - .h1[OBELiX is a curated data set of nearly 600 materials with experimentally measured ionic conductivity], ready for ML use. - Therrien et al. [OBELiX: A curated dataset of crystal structures and experimentally measured ionic conductivities for lithium solid-state electrolytes](https://arxiv.org/abs/2502.14234), Digital Discovery, 2026. -- - We have .h1[compared DFT and ML force fields for the estimation of ionic conductivities] in solid lithium electrolytees: both have similarly weak correlation with experimental values. - Shaaban Kabakibo et al. [A comparative study of molecular dynamics approaches for simulating ionic conductivity in solid lithium electrolytes](https://arxiv.org/abs/2603.28012), AI4Mat, ICML 2026. -- - .h1[Multi-fidelity active learning] with generative models can be effective at exploring large candidate spaces with expensive validation methods. - Hernandez-Garcia, Saxena et al. [Multi-fidelity active learning with GFlowNets](https://arxiv.org/abs/2306.11715). TMLR, 2024 --- ## Acknowledgements .left-column-33[.center[] Paper: [arxiv.org/abs/2603.28012](https://arxiv.org/abs/2603.28012) Funding and support: NRC, Calcul Québec,and the Digital Research Alliance of Canada, NSERC Doctoral program, FRQNT Doctoral research scholarship program and RQMP. ] .right-column-66[.center[]] --- ## Looking for an internship? .center[We look for students interested in .h1[4-6 months (paid!) research internships] to work on ML for materials!] - Dates: September 2026 - March 2027 - Location: Mila in Montreal - Relevant background: - Machine learning basics - Generative modelling (GFlowNets) - Active learning and Bayesian optimisation - MLIPs - DFT - ... - Applications: - Solid-state electrolytes for batteries - Electrocatalysts for HER and OER - General machine learning for materials - ... --- name: cemdi-paims-jul26 class: title, middle  Alex Hernandez-Garcia, Dounia Shaaban Kabakibo, Divya Sharma, Félix Therrien, Lena Podina... .center[
    
    
    
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