Abstract

The consistency of the EFT of two interacting spin-2 fields is checked by applying forward limit positivity bounds on the scattering amplitudes to exclude the region of parameter space devoid of a standard UV completion. We focus on two classes of theories that have the highest possible EFT cutoff, namely those theories modelled on ghost-free interacting theories of a single massive spin-2 field. We find that the very existence of interactions between the spin-2 fields implies more stringent bounds on all the parameters of the EFT, even on the spin-2 self-interactions. This arises for two reasons. First, with every new field included in the low-energy EFT, comes the ‘knowledge’ of an extra pole to be subtracted, hence strengthening the positivity bounds. Second, while adding new fields increases the number of free parameters from the new interactions, this is rapidly overcome by the increased number of positivity bounds for different possible scattering processes. We also discuss how positivity bounds appear to favour relations between operators that effectively raise the cutoff of the EFT.

Highlights

  • In a recent work [1] we considered two classes of effective field theory (EFT) descriptions for interactions of multiple spin-2 fields [2], each based on the requirement that the cutoff of the effective field theory was as high as possible

  • We focus on two classes of theories that have the highest possible EFT cutoff, namely those theories modelled on ghost-free interacting theories of a single massive spin-2 field

  • These EFTs were constructed using the assumption that the symmetry that is spontaneously broken by the mass term is diffeomorphism invariance

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Summary

Introduction

In a recent work [1] we considered two classes of effective field theory (EFT) descriptions for interactions of multiple spin-2 fields [2], each based on the requirement that the cutoff of the effective field theory was as high as possible. These EFTs were constructed using the assumption that the symmetry that is spontaneously broken by the mass term is diffeomorphism invariance. These multiple spin-2 theories are modelled on the successful highest cutoff interacting theory of a single spin-2 field, i.e. ghost-free massive gravity [4]

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