Scattering amplitudes in N=2 Maxwell-Einstein and Yang-Mills/Einstein supergravity

TL;DR

This paper reveals a double-copy structure in N=2 supergravity scattering amplitudes, connecting gauge theories and supergravity, and provides explicit tree-level and one-loop amplitude computations.

Contribution

It demonstrates a double-copy framework for N=2 Maxwell-Einstein and Yang-Mills/Einstein supergravity amplitudes, linking gauge theories to supergravity in four and five dimensions.

Findings

Double-copy structure in supergravity amplitudes

Explicit tree-level and one-loop computations

Compact superamplitude expressions organized by gauge coupling

Abstract

We expose a double-copy structure in the scattering amplitudes of the generic Jordan family of N=2 Maxwell-Einstein and Yang-Mills/Einstein supergravity theories in four and five dimensions. The Maxwell-Einstein supergravity amplitudes are obtained through the color/kinematics duality as a product of two gauge-theory factors; one originating from pure N=2 super-Yang-Mills theory and the other from the dimensional reduction of a bosonic higher-dimensional pure Yang-Mills theory. We identify a specific symplectic frame in four dimensions for which the on-shell fields and amplitudes from the double-copy construction can be identified with the ones obtained from the supergravity Lagrangian and Feynman-rule computations. The Yang-Mills/Einstein supergravity theories are obtained by gauging a compact subgroup of the isometry group of their Maxwell-Einstein counterparts. For the generic Jordan family this process is identified with the introduction of cubic scalar couplings on the bosonic gauge-theory side, which through the double copy are responsible for the non-abelian vector interactions in the supergravity theory. As a demonstration of the power of this structure, we present explicit computations at tree-level and one loop. The double-copy construction allows us to obtain compact expressions for the supergravity superamplitudes which are naturally organized as polynomials in the gauge coupling constant.