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Dr Matthias Wilhelm (NBI)19/08/2026, 10:50Plenary
In this talk, we will present recent progress on applying machine-learning techniques to speed up calculations in theoretical physics, in which we desire exact and analytic results. One example are so-called integration-by-parts reductions of Feynman integrals, which pose a frequent bottleneck in state-of-the-art calculations in theoretical particle and gravitational-wave physics. These...
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Nils Hermansson-Truedsson (University of Edinburgh)19/08/2026, 11:10Plenary
Many low-energy precision tests of hadronic observables in the Standard Model now require the inclusion of isospin-breaking corrections due to light-quark mass differences and electromagnetism (QED). Isospin breaking typically appears for any prediction with better than percent-level precision, where examples are particle decay rates, hadron mass differences and the muon anomalous magnetic...
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Daniel Murnane (Niels Bohr Institute, University of Copenhagen)19/08/2026, 11:30
Reconstruction and simulation at a collider experiment are long chains of specialised algorithms, each tuned to a single step. We ask whether one model can serve many of those steps at once, while still producing the intermediate objects (tracks, calorimeter cells, clusters, particles and jets) that make the chain interpretable. We represent every object in an event in a single shared token...
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Gage DeZoort (Princeton University)19/08/2026, 11:50Plenary
The performance of deep learning models is sensitive to the settings of various hyperparameters, most importantly learning rate and initialization scale. Hyperparameter tuning becomes expensive at scale, motivating the modern paradigm of hyperparameter transfer, a strategy for inferring near-optimal hyperparameters in larger models from their smaller counterparts, which are cheaper to...
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Lukas Liland (TU Dortmund)19/08/2026, 12:10Poster
Any physics experiment consists, in essence, of collecting times, locations and charges. The quantity of interest that the experiment measures must be derived from these three basic ones, for example via a neural network that takes these data as input and produces an estimate of the value in concern as output. However, the true distribution of the quantity in interest is convolved (or folded)...
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Johann Ioannou-Nikolaides (NBI)19/08/2026, 12:15Poster
In many classification problems, reliable instance-level labels are unavailable. However, it is often possible to construct weakly enriched unlabeled samples: datasets selected by different cuts, sources, populations, or experimental conditions that change latent class proportions without revealing them. Classification without Labels (CWoLa) shows that, in the binary case ($K=2$), a classifier...
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Dr Bo Cao (Department of Physics and Astronomy; Nuclear Physics, Uppsala University)19/08/2026, 12:20Poster
We present a Gradient-Boosted Decision Tree (BDT) for $\pi^0$ reconstruction in the $e^+e^- \to \pi^+\pi^-\pi^0\gamma$ process at the KLOE experiment. Trained on Monte Carlo events using ten kinematic variables and a series of preselection criteria (including $\chi^2 < 100$), the model is optimized via Bayesian hyperparameter search. On independent validation samples, the BDT achieves an AUC...
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Stefan Cretu (Lund University)19/08/2026, 12:25Poster
Precise detector alignment is essential for reliable charged-particle tracking in high-energy physics experiments. Standard track-based alignment methods typically depend on iterative global fits which can become computationally demanding for large and highly segmented detectors.
We investigate a machine-learning approach in which detector sensors are represented as nodes in a graph, while...
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