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Download loader/physics.py from fastmachinelearning/hls4ml_lhc_jets_150p: direct link, hf CLI and curl.
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3.77 kB
| # Restricting to the leading constituents and normalising them. | |
| # | |
| # Copied from the study's own data module (jet_tagging_gdl, | |
| # src/data/hls4ml_datamodule.py) rather than rewritten, so that arrays built from the | |
| # record and arrays built from the original h5 files agree bit for bit: the same stable | |
| # argsort over all 150 slots, the same truncate-or-pad, the same python-float scales and | |
| # the same eps. | |
| from pathlib import Path | |
| import numpy as np | |
| # Features that live on both sides of zero, so the scale is half the observed range. | |
| CENTERED_FEATURES = { | |
| "j1_px", "j1_py", "j1_pz", | |
| "j1_eta", "j1_etarel", "j1_etarot", | |
| "j1_phi", "j1_phirel", "j1_phirot", | |
| "j1_costheta", "j1_costhetarel", | |
| } | |
| # Features that are non-negative by construction, so the scale is the observed maximum. | |
| POSITIVE_FEATURES = { | |
| "j1_pt", "j1_ptrel", | |
| "j1_e", "j1_erel", | |
| "j1_deltaR", | |
| } | |
| def restrict_and_sort_by_pt(x, pt_idx: int, nconstituents: int | None) -> np.ndarray: | |
| """Keep the leading *nconstituents* by pT, in descending pT order. | |
| The full constituent list is sorted before truncation, so the constituents kept are | |
| genuinely the highest-pT ones whatever order they appear in on disk. Negating and | |
| using a stable sort gives a deterministic order for equal-pT constituents (ties keep | |
| their on-disk order); ``argsort(...)[::-1]`` would instead reverse an unstable | |
| ascending sort, making tie order arbitrary run to run. Padded slots carry pT = 0 and | |
| therefore sort to the end. | |
| """ | |
| sort_idx = np.argsort(-x[:, :, pt_idx], axis=1, kind="stable") | |
| x = np.take_along_axis(x, sort_idx[:, :, np.newaxis], axis=1) | |
| target = x.shape[1] if (nconstituents is None or nconstituents <= 0) else nconstituents | |
| if x.shape[1] < target: | |
| padding = np.zeros((x.shape[0], target - x.shape[1], x.shape[2]), dtype=x.dtype) | |
| return np.concatenate((x, padding), axis=1) | |
| return x[:, :target, :] | |
| def fit_physics_norm(x_train, feature_names) -> dict[str, tuple[str, float]]: | |
| """One scale per feature, fitted on the restricted training array alone.""" | |
| params: dict[str, tuple[str, float]] = {} | |
| for i, name in enumerate(feature_names): | |
| vals = x_train[:, :, i] | |
| vmin, vmax = float(vals.min()), float(vals.max()) | |
| if name in CENTERED_FEATURES: | |
| params[name] = ("centered", 0.5 * (vmax - vmin)) | |
| elif name in POSITIVE_FEATURES: | |
| params[name] = ("positive", vmax) | |
| else: | |
| raise ValueError(f"Feature '{name}' not categorised in CENTERED or POSITIVE sets.") | |
| return params | |
| def apply_physics_norm(x, feature_names, params, eps: float = 1e-8) -> np.ndarray: | |
| """Divide each feature by its scale. Zero padding stays zero, so it survives.""" | |
| x_norm = x.copy() | |
| for i, name in enumerate(feature_names): | |
| kind, scale = params[name] | |
| if kind not in {"centered", "positive"}: | |
| raise ValueError(f"Unknown normalisation kind '{kind}' for feature '{name}'.") | |
| x_norm[:, :, i] /= (scale + eps) | |
| return x_norm | |
| def save_norm_params(path, params: dict[str, tuple[str, float]]) -> None: | |
| """The study's own npz layout, which its diagnostics and feature lookup read back.""" | |
| names = np.array(list(params.keys()), dtype="U64") | |
| kinds = np.array([params[n][0] for n in names], dtype="U16") | |
| scales = np.array([params[n][1] for n in names], dtype=np.float32) | |
| np.savez(Path(path), feature_names=names, kinds=kinds, scales=scales) | |
| def load_norm_params(path) -> dict[str, tuple[str, float]]: | |
| npz = np.load(Path(path), allow_pickle=False) | |
| return { | |
| str(name): (str(kind), float(scale)) | |
| for name, kind, scale in zip(npz["feature_names"], npz["kinds"], npz["scales"]) | |
| } | |