Abstract

We distinguish between the notions of asymptotic causality and infrared causality for gravitational effective field theories, and show that the latter gives constraints consistent with gravitational positivity bounds. We re-explore the scattering of gravitational waves in a spherically symmetric background in the EFT of gravity in D ≥ 5, for which the leading-order correction to Einstein gravity is determined by the Gauss-Bonnet operator. We reproduce the known result that the truncated effective theory exhibits apparent time advances relative to the background geometry for specific polarisations, which naively signal a violation of causality. We show that by properly identifying the regime of validity of the effective theory, the apparent time advance can be shown to be unresolvable. To illustrate this, we identify specific higher-dimension operators in the EFT expansion which become large for potentially resolvable time advances, rendering the EFT expansion invalid. Our results demonstrate how staying within the confines of the EFT, neither infrared nor asymptotic causality are ever violated for Einstein-Gauss-Bonnet gravity, no matter how low the scale, and furthermore its causality can be understood without appealing to a precise UV completion such as string theory.

Highlights

  • We distinguish between the notions of asymptotic causality and infrared causality for gravitational effective field theories, and show that the latter gives constraints consistent with gravitational positivity bounds

  • We re-explore the scattering of gravitational waves in a spherically symmetric background in the effective field theories (EFTs) of gravity in D ≥ 5, for which the leading-order correction to Einstein gravity is determined by the Gauss-Bonnet operator

  • Our results demonstrate how staying within the confines of the EFT, neither infrared nor asymptotic causality are ever violated for Einstein-Gauss-Bonnet gravity, no matter how low the scale, and its causality can be understood without appealing to a precise UV completion such as string theory

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Summary

Introduction

Relativistic causality is a powerful tool in discriminating between low-energy field theories. The second is to demand analyticity for scattering amplitudes via dispersion relations [8] In recent years the former criterion has become known as asymptotic (sub)luminality [9–14], and the latter has developed into a multitude of positivity bounds which can be used to put powerful constraints on consistent low-energy effective field theories (EFTs) [15–28]. By considering the scalar theory in a fixed Minkowski background (for which ∆T GR = 0), and choosing an analogous spherically symmetric background for the scalar field, we can engineer a situation that closely parallels the EFT of gravity In this case, we find that imposing the bounds implied by the validity of the EFT, it remains possible to engineer a resolvable time advance. The remaining (t, r) indices are indicated by letters at the beginning of the Latin alphabet (a, b, . . . )

Gravitational effective field theories
Black holes in D-dimensional EFT
Metric perturbations
Apparent local superluminality
Scattering phase shifts
Time delays
Time delay for D-dimensional black hole
Constraints on background
Constraints on perturbations
Regime of validity from time delays
Unresolvability of time delay
A casual case of cautionary acausality
Quartic Galileon
Regime of validity
Scattering and time delay
Gravitational positivity bounds from infrared causality
Bound from asymptotic causality
Positivity bound from IR causality
Discussion
A Master variables for metric perturbations
Tensor modes
Vector modes
Scalar modes
B Potentials
Dimension-4 operators
Dimension-6 operators
Dimension-8 operators
D Galileon perturbations
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