Abstract

The Kerr-Schild (KS) formalism is a powerful tool for constructing exact solutions in general relativity. In this paper, we present a generalization of the conventional KS formalism to double field theory (DFT) and supergravities. We introduce a generalized KS ansatz for the generalized metric in terms of a pair of null vectors. Applying this ansatz to the equations of motion of DFT, we construct the generalized KS field equation. While the generalized KS equations are quadratic in the fields, we show that it is possible to find solutions by considering linear equations only. Furthermore, we construct a Killing spinor equation under the generalized KS ansatz. Based on this formalism, we show that the classical double copy structure, which represents solutions of the Einstein equation in terms of solutions of the Maxwell equation, can be extended to the entire massless string NS-NS sector. We propose a supersymmetric classical double copy which shows that solutions of the Killing spinor equation can be realized in terms of solutions of the BPS equation of the supersymmetric Maxwell theory.

Highlights

  • Field equation to a set of linear differential equations

  • We present a generalization of the conventional KS formalism to double field theory (DFT) and supergravities

  • We construct a Killing spinor equation under the generalized KS ansatz. Based on this formalism, we show that the classical double copy structure, which represents solutions of the Einstein equation in terms of solutions of the Maxwell equation, can be extended to the entire massless string NS-NS sector

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Summary

Generalized Kerr-Schild ansatz in DFT

In general relativity (GR) the Kerr-Schild ansatz is a minimal extension of linear perturbation around a background metric g. It is achieved by introducing a null vector l, and the ansatz is given by gμν = gμν + κφlμlν , μ, ν, · · · = 0, 1, · · · d − 1 ,. The main advantage of the Kerr-Schild ansatz is that it preserves some features of the linearized perturbation. The form of the inverse metric and its determinant are gμν = gμν − κφlμlν , det(g) = det(g). We investigate Buscher’s rule and show that the form of the generalized Kerr-Schild ansatz is preserved under T-duality

Linear perturbations of generalized metric
Generalized Kerr-Schild ansatz
Double vielbein
T-duality
Field equations in a flat background
Constructing field equations
Solving the field equations
Classical double copy
Generalization to curved backgrounds
Uplifting to general backgrounds
Equations of motion
Killing spinor equation
M pDM ε
Supersymmetric classical double copy
Chiral null model
F1-NS5 system
Charged black string
Summary
A Conventional Kerr-Schild formalism
Connection and curvature
M pΦMmn
Full Text
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