| --- |
| license: cc-by-4.0 |
| language: |
| - en |
| pretty_name: RADII |
| size_categories: |
| - 10K<n<100K |
| task_categories: |
| - other |
| tags: |
| - materials-science |
| - crystal-structures |
| - generative-models |
| - benchmark |
| - kdd-2026 |
| - nanoparticles |
| configs: |
| - config_name: default |
| data_files: |
| - split: train |
| path: train.parquet |
| - split: id_test |
| path: id_test.parquet |
| - split: ood_test |
| path: ood_test.parquet |
| --- |
| |
| # RADII: Radius-Resolved Benchmark of Nanoparticle Structures |
|
|
| **RADII** measures where graph generative models start to fail as the structures |
| they generate grow larger. Radius is treated as a continuous scaling knob from |
| in-distribution to out-of-distribution; the dataset spans 10 materials and 25 |
| radii with leakage-free splits. |
|
|
| - **Paper:** *How Far Can You Grow? Characterizing the Extrapolation Frontier of Graph Generative Models for Materials Science* — KDD '26 |
| - **Code (models, trainer, generation pipeline):** [github.com/KurbanIntelligenceLab/RADII](https://github.com/KurbanIntelligenceLab/RADII) (MIT) |
| - **Archival DOI:** [10.5281/zenodo.20431021](https://doi.org/10.5281/zenodo.20431021) (CC-BY-4.0) |
|
|
| ## Quick start |
|
|
| ```bash |
| pip install datasets |
| ``` |
|
|
| ```python |
| from datasets import load_dataset |
| |
| ds = load_dataset("KurbanIntelligenceLab/RADII", split="train").with_format("torch") |
| print(ds.features, len(ds), ds[0]["material"], ds[0]["num_atoms"]) |
| ``` |
|
|
| That's it — no `trust_remote_code`, no Zenodo download, no regeneration. |
|
|
| ## Splits |
|
|
| | Split | Size | Radii (Å) | |
| |---|---|---| |
| | `train` | 48,000 | 15 values: 8–10, 12, 14, 16, 18, 20, 22–28 | |
| | `id_test` | 13,500 | 6 values: 11, 13, 15, 17, 19, 21 (interleaved, unseen orientations) | |
| | `ood_test` | 13,480 | 4 values: 6, 7, 29, 30 (strictly outside training range) | |
|
|
| OOD test structures are ~59% smaller and ~24% larger than the smallest and |
| largest training structures (atom counts 33–11,298 vs train 81–9,148). |
|
|
| ## Materials (10) |
|
|
| Ag, Au, CH₃NH₃PbI₃, Fe₂O₃, MoS₂, PbS, SnO₂, SrTiO₃, TiO₂, ZnO. |
|
|
| ## Schema (per row) |
|
|
| | Column | Type | Notes | |
| |---|---|---| |
| | `material` | str | One of the 10 above | |
| | `radius` | int | Truncation radius in Å | |
| | `rot_idx` | int | Orientation index | |
| | `split` | str | `train`, `id_test`, or `ood_test` | |
| | `num_atoms` | int | Length of `pos`/`z` | |
| | `pos` | list[list[float32]] | `num_atoms × 3` atomic coordinates | |
| | `z` | list[int8] | `num_atoms` atomic numbers | |
| | `cell_matrix` | list[list[float32]] | `3 × 3` lattice vectors of the parent unit cell | |
| | `cell_pos` | list[list[float32]] | Unit-cell basis positions (per-material) | |
| | `cell_z` | list[int8] | Unit-cell basis atomic numbers | |
|
|
| ## Analysis recipes (per-radius, per-material, cross-split) |
|
|
| The metadata columns are first-class, so slicing and grouping are one-liners: |
|
|
| ```python |
| from datasets import load_dataset |
| |
| # All three splits at once |
| ds_all = load_dataset("KurbanIntelligenceLab/RADII") |
| |
| # Per-radius slice — every train sample at R=12 |
| r12 = ds_all["train"].filter(lambda x: x["radius"] == 12) |
| |
| # Per-material grouping |
| materials = ds_all["train"].unique("material") # ['Ag', 'Au', ...] |
| ag_ood = ds_all["ood_test"].filter(lambda x: x["material"] == "Ag") |
| |
| # Cross-split: atom counts by radius |
| import pandas as pd |
| for split in ("train", "id_test", "ood_test"): |
| df = ds_all[split].select_columns(["radius", "num_atoms"]).to_pandas() |
| print(split, df.groupby("radius")["num_atoms"].agg(["mean", "min", "max"])) |
| |
| # Atom-count envelope check (replicates the paper's 59% / 24% statistic) |
| train_min, train_max = ds_all["train"]["num_atoms"], ds_all["train"]["num_atoms"] |
| print("train atom-count range:", min(train_min), "to", max(train_max)) |
| print("OOD atom-count range:", min(ds_all["ood_test"]["num_atoms"]), |
| "to", max(ds_all["ood_test"]["num_atoms"])) |
| ``` |
|
|
| ## PyTorch collate (variable-length `pos`/`z`) |
|
|
| ```python |
| import torch |
| from torch.utils.data import DataLoader |
| |
| def collate(batch): |
| return { |
| "pos": [torch.as_tensor(b["pos"]) for b in batch], |
| "z": [torch.as_tensor(b["z"]) for b in batch], |
| "cell_matrix": torch.stack([torch.as_tensor(b["cell_matrix"]) for b in batch]), |
| "material": [b["material"] for b in batch], |
| "radius": torch.tensor([b["radius"] for b in batch]), |
| } |
| |
| loader = DataLoader(ds, batch_size=32, shuffle=True, collate_fn=collate) |
| ``` |
|
|
| For PyTorch Geometric, the `pos`/`z` lists drop straight into |
| `torch_geometric.data.Batch.from_data_list(...)`. |
|
|
| ## Models |
|
|
| The 5 baselines from the paper (ADiT, CDVAE, DiffCSP, FlowMM, MatterGen) live |
| in the GitHub repo's `radii.models` namespace and follow the standard |
| HuggingFace model interface (`PyTorchModelHubMixin`): |
|
|
| ```python |
| from radii.models import ADiTUnitCell |
| from radii.train_config import ModelConfig |
| |
| m = ADiTUnitCell(**ModelConfig.ADiT.to_dict()) |
| m.save_pretrained("./my_adit") |
| m2 = ADiTUnitCell.from_pretrained("./my_adit") |
| # m.push_to_hub("my-username/my-radii-adit") also works |
| ``` |
|
|
| See the GitHub README for training (`python -m radii.train --model adit`) and |
| override flags (`--epochs`, `--lr`, `--from-checkpoint`, `--eval-only`). |
|
|
| ## Citation |
|
|
| ```bibtex |
| @article{polat2026far, |
| title = {How Far Can You Grow? Characterizing the Extrapolation Frontier of Graph Generative Models for Materials Science}, |
| author = {Polat, Can and Serpedin, Erchin and Kurban, Mustafa and Kurban, Hasan}, |
| journal = {arXiv preprint arXiv:2602.09309}, |
| year = {2026} |
| } |
| ``` |
|
|
| ## License |
|
|
| CC-BY-4.0. See [10.5281/zenodo.20431021](https://doi.org/10.5281/zenodo.20431021) |
| for the archival record terms. Accompanying code is MIT-licensed at the GitHub repo. |
|
|