w-boson-regression-eval
Explainable Equivariant Neural Networks for Particle Physics: PELICAN — Bogatskiy et al. (2023) (arXiv:2307.16506, 2023)
What this evaluates
Evaluates a model's ability to reconstruct the 4-momentum and mass of a W-boson from jet constituents, testing regression accuracy and physical consistency under truth-level and detector-simulated (Delphes) conditions. It compares equivariant neural networks against traditional physics-based taggers.
Datasets
- W-boson 4-momentum regression dataset — total ?; splits: test (-1)
Metrics
resolution ($\sigma_{p^{T}}$, $\sigma_{m}$, $\sigma_{\Delta R}$)(primary) — range: percent | centirad- Standard deviation of the relative error between predicted and true values for transverse momentum ($p^T$), mass ($m$), and angular separation ($\Delta R$). Expressed as percentage for $p^T$ and $m$, and centiradians for $\Delta R$.
Input / output format
Input: Set of jet constituents (4-momenta) representing a hadronic jet containing a W-boson decay.
Output: Reconstructed 4-momentum vector of the W-boson ($p^W$) or its mass.
Scoring recipe
def compute_resolution(pred, true):
error = np.abs(pred - true)
resolution = np.std(error) / np.mean(true) * 100
return resolution
Common pitfalls
- Confusing truth-level inputs with detector-simulated (Delphes) inputs, which yield significantly higher resolutions.
- Mixing up 'contained' mass ($p^W_{cont}$) with true mass ($p^W_{true}$) targets, which require different model training objectives.
Evidence (verbatim from paper)
Table 12: PELICAN resolutions for models trained to reconstruct $p^{W}_{\mathrm{true}}$ with variable $W$ mass.
| Method | $\sigma_{p^{T}}$ (%) | $\sigma_{m}$ (%) | $\sigma_{\Delta R}$ (centirad) |
Citation
@misc{bogatskiy2023pelican,
title={Explainable Equivariant Neural Networks for Particle Physics: PELICAN},
author={Bogatskiy et al. (2023)},
year={2023},
note={arXiv:2307.16506}
}
- arXiv: 2307.16506