Oct 5 – 9, 2026
KIT
Europe/Berlin timezone

Session

Track 1 - Analytic integrals

T1
Oct 6, 2026, 11:00 AM
NTI Hörsaal, building 30.10 (KIT)

NTI Hörsaal, building 30.10

KIT

Engesserstr. 5, 76131 Karlsruhe

Conveners

Track 1 - Analytic integrals: Parallel Session II

  • Sven Moch

Presentation materials

There are no materials yet.

  1. Johannes Henn (Max Planck Institute for Physics)
    10/6/26, 11:00 AM
    1

    Precise predictions for cross-sections at present and future particle colliders require reliable methods for evaluating multi-loop Feynman integrals, which are often beyond the reach of direct analytic techniques. In this talk, I will present new numerical approaches that exploit general structural properties of quantum field theory—such as positivity and analyticity—to compute Feynman...

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  2. Qinglin Yang (Max Planck Institute for Physics, Garching, Germany)
    10/6/26, 11:25 AM
    1

    We present a bootstrap construction of planar two-loop six-gluon scattering amplitudes, focusing on the ``most complicated terms'' in the sense of Lipatov. From an analysis of on-shell diagrams, we identify a complete and conformally invariant set of leading singularities. Combining these results with recent advances in understanding the relevant function space and with insights from...

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  3. Christoph Nega (Max Planck Institut für Gravitationsphysik)
    10/6/26, 11:50 AM
    1

    The relationship between unit leading singularities and canonical differential equations has played a central role in modern multi-loop calculations. While this connection is well understood for polylogarithmic integrals, its extension to more general classes of functions has remained unclear.

    In this talk, I will present a generalized notion of leading singularities that naturally extends...

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  4. Hantian Zhang (CERN)
    10/6/26, 12:15 PM
    1

    We propose a second-order partial differential equation method to solve multi-loop Feynman integrals as an equilibrium problem. As a proof-of-concept demonstration, we perform a Galerkin discretization of the corresponding variational form and employ the finite element method to compute two-loop four-point Feynman integrals. This method can solve the integral over a broad region of...

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