| --- |
| license: cc-by-4.0 |
| --- |
| |
| ## Model Summary |
|
|
| This model card provides a DPA3 model[1] trained on the OMol25[2] dataset. We provide one model: |
|
|
| - `DPA3-Omol-Large` – 12 layers, large-scale model for broad molecular chemistry |
|
|
| The model is trained with **charge** and **spin** as input frame parameters, following the OMol25 dataset convention. Here **spin** refers to the **spin multiplicity** (2S+1), not the spin quantum number S. Users can specify `charge` and `spin` when running simulations; if not specified, defaults of `charge=0` and `spin=1` (singlet) are used. |
|
|
| The model is compatible with **DeePMD-kit v3.1.3**. For other installation options, please visit the [Releases page](https://github.com/deepmodeling/deepmd-kit/releases/tag/v3.1.3) to download the off-line package for v3.1.3, and refer to the [official documentation](https://docs.deepmodeling.com/projects/deepmd/en/v3.1.3/install/easy-install.html) for off-line installation instructions. |
|
|
| ## Usage |
|
|
| ### Model Evaluation |
|
|
| Evaluate the model through the dp test command line: |
|
|
| ```bash |
| dp --pt test -m DPA3-Omol-Large.pt -s path_to_your_system |
| ``` |
|
|
| ### ASE Calculator |
|
|
| You can directly use the following Python code for prediction or optimization with standard ASE calculator. |
|
|
| **Charge and spin** can be explicitly specified via `fparam` keyword in `atoms.info`. Note that `spin` here means **spin multiplicity** (2S+1). If not set, the default values `charge=0` and `spin=1` (singlet) will be used. |
|
|
| ```python |
| ## Compute potential energy |
| from ase import Atoms |
| from deepmd.calculator import DP as DPCalculator |
| |
| dp = DPCalculator("DPA3-Omol-Large.pt") |
| |
| # Example: ethanol molecule |
| ethanol = Atoms( |
| "C2H6O", |
| positions=[ |
| (-0.7472, -0.0575, 0.0000), |
| ( 0.7209, 0.0178, 0.0000), |
| ( 1.1431, 1.4297, 0.0000), |
| (-1.1576, -1.0720, 0.0000), |
| (-1.1267, 0.4548, -0.8932), |
| (-1.1267, 0.4548, 0.8932), |
| ( 1.0797, -0.5050, -0.8946), |
| ( 1.0797, -0.5050, 0.8946), |
| ( 2.1108, 1.4520, 0.0000), |
| ], |
| cell=[100, 100, 100], |
| ) |
| |
| # Specify charge and spin multiplicity (optional) |
| # If not set, defaults are charge=0, spin=1 (singlet) |
| ethanol.info.update( |
| {"fparam": [0.0, 1.0]} # charge=0, spin multiplicity=1 (singlet) |
| ) |
| |
| ethanol.calc = dp |
| print(ethanol.get_potential_energy()) |
| print(ethanol.get_forces()) |
| |
| ## Run BFGS structure optimization |
| from ase.optimize import BFGS |
| |
| dyn = BFGS(ethanol) |
| dyn.run(fmax=1e-6) |
| print(ethanol.get_positions()) |
| ``` |
|
|
| ### LAMMPS |
|
|
| Use LAMMPS for molecular dynamics calculation with the DPA3 model, you first need to freeze the *.pt model into a *.pth model using the following command: |
|
|
| ```bash |
| dp --pt freeze -c DPA3-Omol-Large.pt -o DPA3-Omol-Large.pth |
| ``` |
|
|
| Then you can make the following modifications in the LAMMPS script to call the DeePMD-kit interface (also see `potential.md`). |
|
|
| **Charge and spin** are provided via the `fparam` keyword in the order of **charge, spin** (spin = spin multiplicity, 2S+1). If `fparam` is not specified, the default values `0.0 1.0` (charge=0, spin multiplicity=1, i.e. singlet) will be used. |
|
|
| ```bash |
| # With explicit charge and spin multiplicity (e.g., charge=2, multiplicity=1) |
| pair_style deepmd DPA3-Omol-Large.pth fparam 2.0 1.0 |
| pair_coeff * * C H O |
| ``` |
|
|
| ```bash |
| # Without fparam: defaults to charge=0, spin multiplicity=1 |
| pair_style deepmd DPA3-Omol-Large.pth |
| pair_coeff * * C H O |
| ``` |
|
|
| For more details on the `fparam` keyword, see the [DeePMD-kit LAMMPS documentation](https://docs.deepmodeling.com/projects/deepmd/en/stable/third-party/lammps-command.html#pair-style-deepmd). |
|
|
| ## Training Dataset |
|
|
| The model is trained on the **Open Molecules 2025 (OMol25)** dataset[2], a large-scale resource for molecular chemistry ML models introduced by Meta FAIR. OMol25 comprises over **100 million** DFT single-point calculations at the **ωB97M-V/def2-TZVPD** level of theory. |
|
|
| Key characteristics of OMol25: |
|
|
| - **83 elements** across the periodic table |
| - **~83M unique molecular systems**, including small molecules, biomolecules, metal complexes, and electrolytes |
| - System sizes up to **350 atoms** (50 on average) |
| - Diverse charge states (−10 to +10) and spin multiplicities (1 to 11) |
| - Explicit solvation, conformers, and reactive structures |
|
|
| The dataset is organized into four major domains: |
|
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| - **Biomolecules:** protein–ligand, protein–protein, and nucleic acid interactions extracted from BioLiP2 and other structural databases, sampled via classical MD |
| - **Metal Complexes:** diverse monometallic transition metal, main group metal, and lanthanide systems with varied ligands and spin states, generated using the Architector package |
| - **Electrolytes:** aqueous and non-aqueous solutions, ionic liquids, and molten salts, sampled via MD (including Ring Polymer MD for nuclear quantum effects) and electrolyte reactivity networks |
| - **Community:** recomputed existing datasets (ANI-2X, Transition-1X, SPICE2, GEOM, etc.) at consistent ωB97M-V/def2-TZVPD level of theory, plus interpolated reactivity datasets |
|
|
| Compositional splitting ensures that validation and test sets contain out-of-distribution molecular formulas relative to training data. |
|
|
| ## Training Details |
|
|
| We train the **DPA3** model in its large (12-layer) configuration, truncated within LiGS order 2. |
|
|
| ### Model configuration |
|
|
|
|
| | Parameter | Value | |
| | --------- | ----- | |
| | `n_dim` | 256 | |
| | `e_dim` | 256 | |
| | `a_dim` | 256 | |
| | `nlayers` | 12 | |
|
|
| ### Training setup |
|
|
| - **Engine:** DeePMD-kit (`v3.1.0` required) |
| - **Batch size:** `auto:2048` (DeePMD-kit automatic batchsize) |
| - **Hardware:** 32 × NVIDIA A800 GPUs |
| - **Training steps:** 2 million steps |
| - **Learning rate schedule:** Cosine annealing |
| - **Cutoff radii and neighbor selections:** |
| - `e_rcut = 6.0`, `e_rcut_smth = 5.3`, `e_sel = 30` |
| - `a_rcut = 4.5`, `a_rcut_smth = 4.0`, `a_sel = 15` |
|
|
| Other hyperparameters and training details can be found in the DPA3 paper[1]. |
|
|
| ## Performance |
|
|
| ### Accuracy on OMol25 Validation Set |
|
|
| We report energy and force errors on the OMol25 validation set. All values are in **meV** (energy per atom) and **meV/Å** (force). |
|
|
|
|
| | Model | Energy MAE/atom (meV) | Energy RMSE/atom (meV) | Force MAE (meV/Å) | Force RMSE (meV/Å) | |
| | ------------------- | :-------------------: | :--------------------: | :----------------: | :-----------------: | |
| | MACE-OMol-L | 1.917 | 11.727 | 10.690 | 63.754 | |
| | **DPA3-Omol-Large** | 1.328 | 11.347 | 12.362 | 62.934 | |
|
|
| ### Accuracy on LAMBench |
|
|
| We evaluate DPA3-Omol-Large on molecule property calculation tasks from **LAMBench**[3]. The following results compare **DPA3-Omol-Large (ours)** with DPA-3.2-5M and MACE-OMol-L. |
|
|
| #### Ligand Binding |
|
|
|
|
| | Model | RMSE (kcal/mol) | MAE (kcal/mol) | |
| | ------------------- | :-------------: | :------------: | |
| | DPA-3.2-5M | 3.40 | 6.90 | |
| | MACE-OMol-L | 1.75 | 0.84 | |
| | **DPA3-Omol-Large** | 1.29 | 0.65 | |
|
|
| #### TorsionNet500 |
|
|
|
|
| | Model | MAEB (kcal/mol) | MAE (kcal/mol) | RMSE (kcal/mol) | NAHB_h | |
| | ------------------- | :-------------: | :------------: | :-------------: | :----: | |
| | DPA-3.2-5M | 0.47 | 0.29 | 0.43 | 50 | |
| | MACE-OMol-L | 0.23 | 0.14 | 0.23 | 9 | |
| | **DPA3-Omol-Large** | 0.24 | 0.16 | 0.25 | 13 | |
| |
| #### Wiggle150 |
| |
| |
| | Model | RMSE (kcal/mol) | MAE (kcal/mol) | |
| | ------------------- | :-------------: | :------------: | |
| | DPA-3.2-5M | 1.54 | 1.19 | |
| | MACE-OMol-L | 1.18 | 0.89 | |
| | **DPA3-Omol-Large** | 1.25 | 0.94 | |
| |
| #### Reaction Barrier |
| |
| |
| | Model | RMSE (kcal/mol) | MAE (kcal/mol) | |
| | ------------------- | :-------------: | :------------: | |
| | DPA-3.2-5M | 12.37 | 6.30 | |
| | MACE-OMol-L | 3.53 | 2.12 | |
| | **DPA3-Omol-Large** | 12.42 | 3.36 | |
| |
| ## Reference |
| |
| [1] Duo Zhang, Anyang Peng, Chun Cai, Wentao Li, Yuanchang Zhou, Jinzhe Zeng, Mingyu Guo et al. "A Graph Neural Network for the Era of Large Atomistic Models." *arXiv preprint arXiv:2506.01686* (2025). |
| |
| [2] Daniel S. Levine, Muhammed Shuaibi, Evan Walter Clark Spotte-Smith, Michael G. Taylor, Muhammad R. Hasyim, Kyle Michel, Ilyes Batatia et al. "The Open Molecules 2025 (OMol25) Dataset, Evaluations, and Models." *arXiv preprint arXiv:2505.08762* (2025). |
| |
| [3] Anyang Peng, Chun Cai, Mingyu Guo, Duo Zhang, Chengqian Zhang, Wanrun Jiang, Yinan Wang et al. "LAMBench: a benchmark for large atomistic models." *npj Computational Materials* (2026). |