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Add new category containing interstitial benchmarks #337
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| Original file line number | Diff line number | Diff line change |
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@@ -41,3 +41,6 @@ __pycache__/ | |
| ml_peg/app/data/* | ||
| !ml_peg/app/data/onboarding/ | ||
| certs/ | ||
| calculate_rmsd.py | ||
| DB/ | ||
| DB.zip | ||
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@@ -12,5 +12,6 @@ Benchmarks | |
| molecular_crystal | ||
| molecular | ||
| bulk_crystal | ||
| interstitial | ||
| lanthanides | ||
| non_covalent_interactions | ||
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| Original file line number | Diff line number | Diff line change |
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| @@ -0,0 +1,92 @@ | ||
| ============ | ||
| Interstitial | ||
| ============ | ||
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| FE1SIA | ||
| ====== | ||
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| Summary | ||
| ------- | ||
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| This benchmark evaluates the formation energies of a single self-interstitial atom (SIA) in a host lattice. The test includes formation energies for distinct configurations within a supercell. | ||
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| Metrics | ||
| ------- | ||
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| 1. RMSD | ||
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| Root Mean Square Deviation of formation energies compared to DFT data. | ||
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| The formation energy of a configuration :math:`E_f` is calculated as: | ||
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| .. math:: | ||
| E_f = E_{config} - \frac{N_{config}}{N_{bulk}} E_{bulk} | ||
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| where :math:`E_{config}` is the total energy of the interstitial configuration containing :math:`N_{config}` atoms, and :math:`E_{bulk}` is the energy of the perfect bulk supercell consisting of :math:`N_{bulk}` atoms. | ||
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| The reference formation energies are derived from DFT calculations provided in the dataset. | ||
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| Computational cost | ||
| ------------------ | ||
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| Low: The geometries are static, requiring only single-point energy calculations for the configurations and the bulk reference. | ||
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| Data availability | ||
| ----------------- | ||
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| Input structures: | ||
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| * Subset ``formation_energy`` of the DFT dataset. | ||
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| * A. Allera, A. M. Goryaeva, P. Lafourcade, J.-B. Maillet, and M.-C. Marinica, | ||
| Neighbors map: An efficient atomic descriptor for structural analysis, | ||
| Computational Materials Science 231 (2024). | ||
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| Reference data: | ||
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| * Computed from the subset ``formation_energy`` of the DFT dataset as input structures. | ||
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| Relastab | ||
| ======== | ||
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| Summary | ||
| ------- | ||
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| This benchmark evaluates the ability of models to correctly rank the stability of different interstitial configurations. It focuses on the relative energy ordering of distinct interstitial structures in the dataset. | ||
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| Metrics | ||
| ------- | ||
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| 1. Kendall Tau | ||
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| Kendall rank correlation coefficient (:math:`\tau`): a measure of rank correlation that evaluates the similarity of the orderings of the data. It assesses the number of *concordant* and *discordant* pairs of observations. For every pair of configurations, it checks if the model agrees with the reference on which is more stable. | ||
| A value of 1.0 indicates perfect agreement, 0.0 indicates no correlation, and -1.0 indicates perfect inversion. | ||
| This metric is sensitive to **pairwise ordering** errors. It is particularly robust for small datasets and focuses strictly on whether the relative stability order is preserved. | ||
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| 2. Spearman | ||
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| Spearman rank correlation coefficient (:math:`\rho`): a non-parametric measure of rank correlation. | ||
| It is defined as the Pearson correlation coefficient between the *rank variables*. It converts raw energies to integer ranks and calculates the linear correlation between them. | ||
| Like Kendall Tau, values range from -1 to 1. An absolute value of 1 indicates a perfect monotonic function. | ||
| While both metrics evaluate ranking, Spearman assesses the general **monotonic relationship**, while Kendall Tau assesses the probability of correct pairwise discrimination. | ||
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| Computational cost | ||
| ------------------ | ||
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| Low: Requires single-point energy calculations for each configuration in the dataset. | ||
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| Data availability | ||
| ----------------- | ||
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| Input structures: | ||
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| * Subset ``relative_stability`` of the DFT dataset. | ||
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| * A. Allera, A. M. Goryaeva, P. Lafourcade, J.-B. Maillet, and M.-C. Marinica, | ||
| Neighbors map: An efficient atomic descriptor for structural analysis, | ||
| Computational Materials Science 231 (2024). | ||
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| Reference data: | ||
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| * Computed from the subset ``relative_stability`` of the DFT dataset as input structures. |
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| """Analyse FE1SIA benchmark.""" | ||
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| from __future__ import annotations | ||
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| from pathlib import Path | ||
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| from ase.io import read, write | ||
| import pytest | ||
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| from ml_peg.analysis.utils.decorators import build_table, plot_parity | ||
| from ml_peg.analysis.utils.utils import load_metrics_config, rmse | ||
| from ml_peg.app import APP_ROOT | ||
| from ml_peg.calcs import CALCS_ROOT | ||
| from ml_peg.models.get_models import get_model_names | ||
| from ml_peg.models.models import current_models | ||
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| MODELS = get_model_names(current_models) | ||
| # D3_MODEL_NAMES = build_d3_name_map(MODELS) | ||
| D3_MODEL_NAMES = {m: m for m in MODELS} | ||
| CALC_PATH = CALCS_ROOT / "interstitial" / "FE1SIA" / "outputs" | ||
| OUT_PATH = APP_ROOT / "data" / "interstitial" / "FE1SIA" | ||
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| METRICS_CONFIG_PATH = Path(__file__).with_name("metrics.yml") | ||
| DEFAULT_THRESHOLDS, DEFAULT_TOOLTIPS, DEFAULT_WEIGHTS = load_metrics_config( | ||
| METRICS_CONFIG_PATH | ||
| ) | ||
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| def get_system_names() -> list[str]: | ||
| """ | ||
| Get list of FE1SIA system names. | ||
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| Returns | ||
| ------- | ||
| list[str] | ||
| List of system names. | ||
| """ | ||
| system_names = [] | ||
| # Try to find names from one of the models | ||
| for model_name in MODELS: | ||
| model_dir = CALC_PATH / model_name | ||
| if model_dir.exists(): | ||
| xyz_files = sorted(model_dir.glob("*.xyz")) | ||
| for xyz in xyz_files: | ||
| if xyz.stem != "ref": | ||
| system_names.append(xyz.stem) | ||
| if system_names: | ||
| break | ||
| return system_names | ||
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| @pytest.fixture | ||
| @plot_parity( | ||
| filename=OUT_PATH / "figure_energy.json", | ||
| title="FE1SIA Formation Energies", | ||
| x_label="Predicted Formation Energy / eV", | ||
| y_label="Reference Formation Energy / eV", | ||
| hoverdata={ | ||
| "System": get_system_names(), | ||
| }, | ||
| ) | ||
| def formation_energies() -> dict[str, list]: | ||
| """ | ||
| Get formation energies for FE1SIA systems. | ||
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| Returns | ||
| ------- | ||
| dict[str, list] | ||
| Dictionary of reference and predicted formation energies. | ||
| """ | ||
| results = {"ref": []} | {mlip: [] for mlip in MODELS} | ||
| ref_stored = False | ||
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| for model_name in MODELS: | ||
| model_dir = CALC_PATH / model_name | ||
| if not model_dir.exists(): | ||
| continue | ||
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| # Load bulk (ref) | ||
| # Note: We rely on calc script having produced ref.xyz | ||
| bulk_path = model_dir / "ref.xyz" | ||
| if not bulk_path.exists(): | ||
| # If bulk is missing, we can't compute formation energy properly | ||
| print(f"Warning: Bulk reference not found for {model_name}") | ||
| continue | ||
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| bulk_atoms = read(bulk_path) | ||
| e_bulk = bulk_atoms.get_potential_energy() | ||
| n_bulk = len(bulk_atoms) | ||
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| xyz_files = sorted(model_dir.glob("*.xyz")) | ||
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| for xyz_file in xyz_files: | ||
| if xyz_file.name == "ref.xyz": | ||
| continue | ||
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| atoms = read(xyz_file) | ||
| e_config = atoms.get_potential_energy() | ||
| n_config = len(atoms) | ||
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| # Predicted formation energy | ||
| # E_f = E_config - (N_config / N_bulk) * E_bulk | ||
| pred_fe = e_config - (n_config / n_bulk) * e_bulk | ||
| # print(model_name, pred_fe) | ||
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| results[model_name].append(pred_fe) | ||
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| # Copy individual structure files to app data directory | ||
| structs_dir = OUT_PATH / model_name | ||
| structs_dir.mkdir(parents=True, exist_ok=True) | ||
| write(structs_dir / xyz_file.name, atoms) | ||
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| if not ref_stored: | ||
| results["ref"].append(atoms.info["ref"]) | ||
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| ref_stored = True | ||
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| return results | ||
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| @pytest.fixture | ||
| def fe_errors(formation_energies) -> dict[str, float]: | ||
| """ | ||
| Get RMSE for formation energies. | ||
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| Parameters | ||
| ---------- | ||
| formation_energies | ||
| Dictionary of reference and predicted formation energies. | ||
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| Returns | ||
| ------- | ||
| dict[str, float] | ||
| Dictionary of RMSEs for all models. | ||
| """ | ||
| results = {} | ||
| for model_name in MODELS: | ||
| if formation_energies.get(model_name): | ||
| results[model_name] = rmse( | ||
| formation_energies["ref"], formation_energies[model_name] | ||
| ) | ||
| # print(f"FE1SIA RMSD for {model_name}: {results[model_name]:.6f} eV") | ||
| # print(formation_energies["ref"], formation_energies[model_name]) | ||
| else: | ||
| results[model_name] = None | ||
| return results | ||
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| @pytest.fixture | ||
| @build_table( | ||
| filename=OUT_PATH / "fe1sia_metrics_table.json", | ||
| metric_tooltips=DEFAULT_TOOLTIPS, | ||
| thresholds=DEFAULT_THRESHOLDS, | ||
| mlip_name_map=D3_MODEL_NAMES, | ||
| ) | ||
| def metrics(fe_errors: dict[str, float]) -> dict[str, dict]: | ||
| """ | ||
| Get all FE1SIA metrics. | ||
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| Parameters | ||
| ---------- | ||
| fe_errors | ||
| RMSE errors for all systems. | ||
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| Returns | ||
| ------- | ||
| dict[str, dict] | ||
| Metric names and values for all models. | ||
| """ | ||
| return { | ||
| "RMSD": fe_errors, | ||
| } | ||
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| def test_fe1sia_analysis(metrics: dict[str, dict]) -> None: | ||
| """ | ||
| Run FE1SIA analysis test. | ||
|
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| Parameters | ||
| ---------- | ||
| metrics | ||
| All FE1SIA metrics. | ||
| """ | ||
| return |
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| Original file line number | Diff line number | Diff line change |
|---|---|---|
| @@ -0,0 +1,7 @@ | ||
| metrics: | ||
| RMSD: | ||
| good: 0.0 | ||
| bad: 30.0 | ||
| unit: eV | ||
| tooltip: "Root Mean Square Deviation of formation energies" | ||
| level_of_theory: DFT |
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I don't think we should need any of these?