Abstract

We study gravitational shock waves using scattering amplitude techniques. After first reviewing the derivation in General Relativity as an ultrarelativistic boost of a Schwarzschild solution, we provide an alternative derivation by exploiting a novel relation between scattering amplitudes and solutions to Einstein field equations. We prove that gravitational shock waves arise from the classical part of a three point function with two massless scalars and a graviton. The region where radiation is localized has a distributional profile and it is now recovered in a natural way, thus bypassing the introduction of singular coordinate transformations as used in General Relativity. The computation is easily generalized to arbitrary dimensions and we show how the exactness of the classical solution follows from the absence of classical contributions at higher loops. A classical double copy between gravitational and electromagnetic shock waves is also provided and for a spinning source, using the exponential form of three point amplitudes, we infer a remarkable relation between gravitational shock waves and spinning ones, also known as gyratons. Using this property, we infer a family of exact solutions describing gravitational shock waves with spin. We then compute the phase shift of a particle in a background of shock waves finding agreement with an earlier computation by Amati, Ciafaloni and Veneziano for particles in the high energy limit. Applied to a gyraton, it provides a result for the scattering angle to all orders in spin.

Highlights

  • JHEP11(2020)160 led to the computation at second order in GN of the Schwarzschild1 and Kerr-Newman solution [75,76,77,78]

  • We have derived a relation between perturbative solutions to Einstein field equations and off-shell scattering amplitudes thanks to a covariant framework developed by Kosower, Maybee and O’Connell [4]

  • We have studied to which gravitational field corresponds a scattering amplitude with an off-shell graviton and two massless particles finding that the latter describes a gravitational shock wave known as Aichelburg-Sexl metric [65]

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Summary

The Aichelburg-Sexl metric

Aichelburg and Sexl derived for the first time an exact solution to Einstein field equations describing the gravitational field generated by a massless particle [65] Their procedure employed the use of an ultrarelativistic boost of a Schwarzschild solution, previously used by D’Eath to address the scattering of two ultrarelativistic black holes [87]. The line element assumes the usual form of an impulsive pp-wave ds2 = dt 2 − dx 2 − dy 2 − dz 2 + 4pGN δ(t − x ) log(y 2 + z 2)(dt − dx ) (2.9) The latter defines a global solution given by two copies of Minkwoski space connected by a singularity along a light cone coordinate. From the computation of the associated Einstein tensor we can infer that the energy momentum tensor is that of a massless particle, confirming the physical interpretation of the metric

Gravitational shock waves from scattering amplitudes
A classical double copy for gravitational shock waves
Spinning gravitational shock waves
The scattering angle in the high energy limit
Conclusion
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