Periodic Reporting for period 1 - LoCoMotive (Loop Corrections from the Theory of Motives)
Reporting period: 2023-01-01 to 2025-06-30
The goals of the project LoCoMotive is to develop new technique beyond the state of the art for the computation of scattering amplitudes based on novel ideas from modern mathematics. In order to achieve its goals, the activities of LoCoMotive are divided into 3 main areas. First, we will perform in in-depth study of the areas of mathematics needed to describe scattering amplitudes, and will develop the relevant mathematics further where needed. Second, we aim at studying scattering amplitudes in a variety of physics theories which exhibit additional symmetries, in order to identify new structures and results in these theories. Finally, we aim at performing very precise predictions for experiments that are out of reach with conventional techniques, in particular collider experiments like the Large Hadron Collider (LHC) at CERN and its possible successors.
Duhr and Porkert and collaborators have used techniques from Calabi-Yau geometry to compute new results for various Yangian-invariant traintrack integrals in two space-time dimensions.
Zhang and collaborators have bootstrapped new results for two-loop integrals that evaluate to non-polylogarithmic functions.
We have computed novel results for various integrals of phenomenological relevance involving massive particles. In particular, Duhr and collaborators have computed the complete two-loop corrections to Bhabha scattering in Quantum Electrodynamics (QED) with the full dependence on the electron mass. This computation has been an open problem for more than a decade. Together with his collaborators, he has also computed for the first time the three-loop QED corrections to the electron self-energy. Chaubey and collaborators have computed for the first time integrals relevant for light-by0light scattering, and in collaboration with Maggio, she has computed a highly non-trivial non-planar family of four-point functions depending on a massive propagator.