Lepton-pair scattering with an off-shell and an on-shell photon at two loops in massless QED
Simon Badger, Jakub Kryś, Ryan Moodie, Simone Zoia
TL;DR
This work addresses the need for precise two-loop QED corrections to electron–muon scattering at the MUonE experiment by computing massless-lepton helicity amplitudes for $0\to \ell\bar{\ell}\gamma\gamma^*$ and expressing the four-point master integrals in a basis of algebraically independent multiple polylogarithms. The authors employ finite-field techniques and a canonical differential-equation framework to reconstruct analytic amplitudes from numerical samples, yielding a compact MPL representation up to weight four for all relevant integral families with a single off-shell leg. They organize the amplitude into gauge-invariant subamplitudes, project onto a four-vector basis, and handle all permutations of integral topologies with an optimized IBP reduction workflow and a momentum-twistor parametrisation for kinematics, including appropriate UV renormalisation and IR factorisation. The resulting analytic expressions and master-integral basis enable efficient, stable two-loop computations that feed N$^3$LO predictions for $e\mu\to e\mu$ and related ISR/RSV observables, contributing directly to MUonE's precision program.
Abstract
We compute the two-loop QED helicity amplitudes for the scattering of a lepton pair with an off-shell and an on-shell photon, $0\to\ell\bar\ellγγ^*$, using the approximation of massless leptons. We express all master integrals relevant for the scattering of four massless particles with a single external off-shell leg up to two loops in a basis of algebraically independent multiple polylogarithms, which guarantees an efficient numerical evaluation and compact analytic representations of the amplitudes. Analytic forms of the amplitudes are reconstructed from numerical evaluations over finite fields. Our results complete the amplitude-level ingredients contributing to the N$^3$LO predictions of electron-muon scattering $eμ\to eμ$, which are required to meet the precision goal of the future MUonE experiment.
