Dual superconformal symmetry of scattering amplitudes in N=4 super-Yang-Mills theory
J. M. Drummond, J. Henn, G. P. Korchemsky, E. Sokatchev
TL;DR
Drummond, Henn, Korchemsky, and Sokatchev demonstrate a dual superconformal symmetry for planar N=4 SYM amplitudes by embedding them in dual superspace. They show manifest dual superconformal covariance for tree-level MHV and NMHV amplitudes, construct compact NMHV tree-level and one-loop NMHV formulas via three-point invariants, and derive anomalous Ward identities governing loop corrections. Infrared divergences break dual conformal invariance, but the finite ratio functions between non-MHV and MHV amplitudes remain dual conformal invariant, a property illustrated explicitly for six points. The framework unifies on-shell superspace, dual superspace, and dual superconformal generators, and points toward connections with Wilson-loop duality and possible twistor-space interpretations, suggesting broad applicability across all N^kMHV amplitudes and couplings.
Abstract
We argue that the scattering amplitudes in the maximally supersymmetric N=4 super-Yang-Mills theory possess a new symmetry which extends the previously discovered dual conformal symmetry. To reveal this property we formulate the scattering amplitudes as functions in the appropriate dual superspace. Rewritten in this form, all tree-level MHV and next-to-MHV amplitudes exhibit manifest dual superconformal symmetry. We propose a new, compact and Lorentz covariant formula for the tree-level NMHV amplitudes for arbitrary numbers and types of external particles. The dual conformal symmetry is broken at loop level by infrared divergences. However, we provide evidence that the anomalous contribution to the MHV and NMHV superamplitudes is the same and, therefore, their ratio is a dual conformal invariant function. We identify this function by an explicit calculation of the six-particle amplitudes at one loop. We conjecture that these properties hold for all, MHV and non-MHV, superamplitudes in N=4 SYM both at weak and at strong coupling.
