Heterotic Kerr-Schild Double Field Theory and its double Yang-Mills formulation

Abstract

We present a formulation of heterotic Double Field Theory (DFT), where the fundamental fields are in O(D, D) representations. The theory is obtained splitting an O(D, D + K ) duality invariant DFT. This procedure produces a Green-Schwarz mechanism for the generalized metric, and a fundamental gauge field which transforms as a gauge connection only to leading order. After parametrization, the former induces a non-covariant transformation on the metric tensor, which can be removed considering field redefinitions, and an ordinary Green-Schwarz mechanism on the b-field. Within this framework we explore perturbative properties of heterotic DFT. We use a relaxed version of the generalized Kerr-Schild ansatz (GKSA), where the generalized background metric is perturbed up to quadratic order considering a single null vector and the gauge field is linearly perturbed before parametrization. Finally we compare the dynamics of the gauge field and the generalized metric in order to inspect the behavior of the classical double copy correspondence at the DFT level.

Einstein-Maxwell theory and the Weyl double copy

“…Such extensions have been considered in the context of the perturbative double copy; however, the exact Kerr-Schild double copy for pure Einstein gravity has difficulty describing an additional massless NS-NS field like a Kalb-Ramond field or a dilaton using the single-null congruence in the conventional Kerr-Schild ansatz. To understand the double copy of such fields in a nonperturbative way, the Kerr-Schild framework was generalized to describe double-field theory and supergravities in [52,53] (see also the extensions [54][55][56]). It would be interesting to try to incorporate such fields using the sourced Weyl double copy, and compare to the spinorial representation of the torsionful Riemann curvature introduced in [37] to study solutions of the universal massless sector of supergravity.…”