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| license: cc-by-4.0 # TODO: confirm — placeholder, common choice for open MLIP releases (e.g. MACE-OFF/MACE-MP). Change if you want something else. | |
| tags: | |
| - deepmd-kit | |
| - molecular-dynamics | |
| - interatomic-potential | |
| - materials-science | |
| - battery-materials | |
| - cathode-material | |
| - layered-oxide | |
| - lithium-ion-battery | |
| - nmc | |
| # NMC622 — LiNi₀.₆Mn₀.₂Co₀.₂O₂ Cathode (DeepMD) | |
|  | |
| ## What this is | |
| DeepMD-kit potentials for **NMC622** (LiNi₀.₆Mn₀.₂Co₀.₂O₂), a layered-oxide | |
| Li-ion cathode material — one of the most widely used commercial cathode | |
| chemistries, here used to study Li-ion diffusion in the layered structure. | |
| ## Transport properties | |
| | | AIMD | MLMD (DeepMD) | | |
| |---|---|---| | |
| | D (Li⁺, cm²/s) | 9.0×10⁻¹² | 2.58×10⁻¹¹ (300K) / 5.12×10⁻¹¹ (600K) | | |
| | Eₐ (eV) | 0.34 | 0.035 | | |
| Mechanical: E = 200 GPa, ν = 0.30, ρ = 4.7 g/cm³. | |
| ## Files & Validation | |
| | File | RMSE energy (eV/atom) | RMSE force (eV/Å) | Training steps | Size | | |
| |---|---|---|---|---| | |
| | `model/nmc622_production.pb` | 0.00239 | 0.166 | 1,000,000 | 450.6 MB | | |
| | `model/nmc622_model1.pb` | 0.00226 | 0.178 | 1,000,000 | 407.6 MB | | |
| *RMSE values are validation-set (held-out) energy/force error, read directly from each run's DeepMD-kit `lcurve.out` at its final training step — not re-derived or estimated.* | |
|  | |
| **2 of 3** current production potentials, the pair with the lowest | |
| validation force RMSE; several earlier iterations (6k/11k/22k-atom | |
| cell-size scans, memory-optimization variants) exist in the source tree as | |
| superseded intermediates and aren't included here. | |
| ## Training pipeline | |
| AIMD random-structure sampling (VASP, PBE, 500K) → DeepMD-kit train/freeze/ | |
| compress. Produced by HPCA (github.com/selvachandrasekaranselvaraj/hpca). | |
| ## Citation | |
| Selva Chandrasekaran Selvaraj, University of Illinois Chicago. Continuum | |
| transport model parameters per Ncube et al. 2026. | |