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Machine-learned interatomic potential models for practical applications Tim Mueller Johns Hopkins University Funded by the Toyota Motor Corporation and the Office of Naval Research Contributors Chuhong Wang Adarsh Balasubramanian Simon Mason


  1. Machine-learned interatomic potential models for practical applications Tim Mueller Johns Hopkins University Funded by the Toyota Motor Corporation and the Office of Naval Research

  2. Contributors Chuhong Wang Adarsh Balasubramanian Simon Mason Alberto Hernandez

  3. Machine-learned interatomic potentials

  4. Machine-learned interatomic potentials

  5. Moment tensor potentials The energy is a polynomial of inner products of vectors between atoms and the vector lengths. A. V. Shapeev, Multiscale Model. Simul., 14(3), 1153–1173.

  6. Moment tensor potentials The energy is a polynomial of inner products of vectors between atoms and the vector lengths. A. V. Shapeev, Multiscale Model. Simul., 14(3), 1153–1173.

  7. Moment tensor potentials The energy is a polynomial of inner products of vectors between atoms and the vector lengths. A. V. Shapeev, Multiscale Model. Simul., 14(3), 1153–1173.

  8. Moment tensor potentials The energy is a polynomial of inner products of vectors between atoms and the vector lengths. They demonstrate excellent balance between speed and interpolative predictive accuracy. Y. Zuo et al., The Journal of Physical Chemistry A 124, 4, 731–745 (2020)

  9. Lithium-ion batteries Anode Material Li + e - Cathode Material

  10. Lithium-ion batteries e - Cathode Material Anode Material Solid-state electrolyte

  11. Lithium-ion batteries Anode Material Anode coating electrolyte Solid-state e - Cathode coating Cathode Material

  12. Lithium-ion batteries In the anode and cathode, lithium ions typically diffuse by hopping into vacant sites. The activation energy can be calculated using the nudged elastic band method. Cathode Material Cathode coating Anode Material Anode coating Solid-state electrolyte

  13. Lithium-ion batteries Diffusion in these materials typically occurs via concerted lithium motion. Cathode Material Cathode coating Anode Material Anode coating Solid-state electrolyte

  14. Concerted lithium-ion diffusion ) C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  15. Lithium-ion batteries In the superionic conductors used as electrolytes, diffusivity can be calculated using ab-initio molecular dynamics. Cathode Material Cathode coating Anode Material Anode coating Solid-state electrolyte

  16. Lithium-ion batteries These do not need to be superionic conductors. Diffusion is too slow for ab initio molecular dynamics. Cathode Material Cathode coating Anode Material Anode coating Solid-state electrolyte

  17. Ensuring high accuracy Moment tensor potentials can be highly accurate for local configurations similar to ones used to train them. C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  18. Ensuring high accuracy Moment tensor potentials can be highly accurate for local configurations similar to ones used to train them. Sometimes a configuration unlike any in the training set is encountered. C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  19. Learning on the fly Moment tensor potentials can be highly accurate for local configurations similar to ones used to train them. When encountering a new configuration, potentials can “learn on the fly”: the new configuration is automatically added to the training data and the potential is retrained to ensure accuracy. C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  20. Learning on the fly Moment tensor potentials can be highly accurate for local configurations similar to ones used to train them. When encountering a new configuration, potentials can “learn on the fly”: the new configuration is automatically added to the training data and the potential is retrained to ensure accuracy. The resulting potential generates molecular dynamics data seven orders of magnitude faster than ab-initio molecular dynamics with nearly the same accuracy. C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  21. Better Arrhenius plots C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  22. Better experimental validation Computed activation energy Mean absolute error = 0.13 eV Mean absolute error = 0.32 eV Experimental activation energy C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  23. New candidate coating materials Li₃B₇O₁₂ Solid-state electrolytes Coating Cathodes Li 7 P 3 S 12 Li₃B₇O₁₂ LiCoO 2 Li 10 GeP 2 S 12 LiFePO 4 Li 10 SnP 2 S 12 Eₐ = 0.56 eV LiMn 2 O 4 Li 10 SiP 2 S 12 Li(MnNiCo) 1/3 O 2 Li 6 PS 5 Br LiMn 1.5 Ni 0.5 O 2 Li 6 PS 5 Cl Li₃Sc₂(PO₄)₃ Solid-state electrolytes Coating Cathodes Li 7 P 3 S 12 Li₃Sc₂(PO₄)₃ LiFePO 4 Li(MnNiCo) 1/3 O 2 Eₐ = 0.64 eV C. Wang, K. Aoyagi, P. Wisesa, and T. Mueller, Chemistry of Materials 32 , 9, 3741–3752 (2020)

  24. Speed considerations Moment tensor potentials are among the fastest machine-learned interatomic potential models, but they are still 1-2 orders of magnitude slower than widely-used physics-derived models like the embedded atom method.

  25. Supervised machine learning

  26. Supervised machine learning 1. Select a hypothesis space Functions that can be created by combining addition subtraction, multiplication, division, exponentiation, distance, sum over neighbors, constant values.

  27. Supervised machine learning 1. Select a hypothesis space Functions that can be created by combining addition subtraction, multiplication, division, exponentiation, distance, sum over neighbors, constant values.

  28. Supervised machine learning 1. Select a hypothesis space Functions that can be created by combining addition subtraction, multiplication, division, exponentiation, distance, sum over neighbors, constant values. Many physics-derived models exist in this hypothesis space: Coulomb, Lennard-Jones, harmonic potentials, embedded atom method, bond order potentials…

  29. Supervised machine learning 1. Select a hypothesis space Functions that can be created by combining addition subtraction, multiplication, division, exponentiation, distance, sum over neighbors, constant values. Functions are represented × E = mc 2 as trees. m ^ c 2

  30. Supervised machine learning 2. Select an objective function

  31. Supervised machine learning 2. Select an objective function Find candidates on convex hull with respect to • Fitness Based on errors with respect to standardized energies, forces, and virial stresses.

  32. Supervised machine learning 2. Select an objective function Find candidates on convex hull with respect to • Fitness • Speed Faster models can handle larger time and length scales.

  33. Supervised machine learning 2. Select an objective function Find candidates on convex hull with respect to • Fitness • Speed • Complexity Simpler models are less likely to overfit training data.

  34. Why do we care about complexity?

  35. Supervised machine learning 3. Search the hypothesis space

  36. Supervised machine learning 3. Search the hypothesis space This problem is known as “symbolic regression”.

  37. Supervised machine learning 3. Search the hypothesis space This problem is known as “symbolic regression”. We use an approach called “genetic programming”, in which functions evolve using an evolutionary algorithm.

  38. Evolutionary step: Crossover       (1 r ) 14 ( r 11)* (3 r )

  39. Evolutionary step: Crossover       (1 r ) 14 ( r 11)* (3 r )

  40. Evolutionary step: Crossover      (1 r ) 14 (3 r )

  41. Evolutionary step: Mutation   (1 r )

  42. Evolutionary step: Mutation   (1 r )

  43. Evolutionary step: Mutation   (1 r )

  44. Evolutionary step: Mutation  r  ( 1)

  45. Evolutionary step: Mutation  r  ( 1) We use conjugate gradient and CMA- ES to optimize the parameters.

  46. Regenerating the embedded atom method Potential model used to generate training data   0.5   6 44.52 527. 6 2         V  SC   9 6 r r     i j j (Sutton and Chen, Philosophical Magazine Letters, 1990)

  47. Regenerating the embedded atom method Potential model used to generate training data   0.5   6 44.52 527. 6 2         V  SC   9 6 r r     i j j (Sutton and Chen, Philosophical Magazine Letters, 1990) Potential model found by genetic programming      0.50                      9.00 6.00 V 0.73 2.53 0.66(384.39) r 0.25 / 20.63 r                  i  j j    A. Hernandez, A. Balasubramanian, F. Yuan, S. A. M. Mason and T. Mueller npj Computational Materials 5 , 112 (2019)

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