Abstract

Within the standard effective field theory of General Relativity, we show that the speed of gravitational waves deviates, ever so slightly, from luminality on cosmological and other spontaneously Lorentz-breaking backgrounds. This effect results from loop contributions from massive fields of any spin, including Standard Model fields, or from tree level effects from massive higher spins $s \ge 2$. We show that for the choice of interaction signs implied by S-matrix and spectral density positivity bounds suggested by analyticity and causality, the speed of gravitational waves is in general superluminal at low-energies on NEC preserving backgrounds, meaning gravitational waves travel faster than allowed by the metric to which photons and Standard Model fields are minimally coupled. We show that departure of the speed from unity increases in the IR and argue that the speed inevitably returns to luminal at high energies as required by Lorentz invariance. Performing a special tuning of the EFT so that renormalization sensitive curvature-squared terms are set to zero, we find that finite loop corrections from Standard Model fields still lead to an epoch dependent modification of the speed of gravitational waves which is determined by the precise field content of the lightest particles with masses larger than the Hubble parameter today. Depending on interpretation, such considerations could potentially have far-reaching implications on light scalar models, such as axionic or fuzzy cold dark matter.

Highlights

  • In this new era of gravitational wave astronomy, it is especially important to understand how gravitational waves propagate

  • effective field theory (EFT) coefficients, the light cone inferred from the low energy sound speed of matter always lies inside the light cone of gravitational waves and is never exactly at the same speed

  • In particular we show that the low energy speed of the gravitational wave depends on the field content of the high-energy completion, and on the spin of the lightest massive particle that is integrated out to derive the low energy Wilsonian action

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Summary

INTRODUCTION

In this new era of gravitational wave astronomy, it is especially important to understand how gravitational waves propagate. (v) Our results remain valid when considering purely quartic curvature corrections, such as those known to arise in the low energy string theory effective action, for which gravitational waves travel superluminally on NEC preserving backgrounds. EFT coefficients (either as inferred from explicit integration of fields or from positivity bounds or as implied from string theory), the light cone inferred from the low energy sound speed of (minimally coupled) matter always lies inside the light cone of gravitational waves and is never exactly at the same speed. We explore the leading curvature-squared contributions to the low energy EFT for gravity in Sec. III and identify their effect on the speed of gravitational waves on FLRW and on static warped backgrounds. As is standard, slightly abuse the EFT operator counting terminology and refer to Riemannn operators as dimension-2n operators evvaerinouthsoduigmhetnhseiyoninscPludkehaknð∂in2hfiÞnni=teMnkPuþlm3nb−e4r of operators þ Á Á Á

EFFECTS OF HEAVY MODES ON GRAVITY AT LOW ENERGY
Effective field theory for gravity at low energy
Tree level interactions
Loop level interactions
Wilsonian effective action
Inclusion of light loops
A word of caution on field redefinitions
Taking care of the dimension-four curvature operators
Relevance of the dimension-six curvature operators
Reorganizing EFT expansion
Identifying the speed
Dimension-four curvature operators
Tensor modes on FLRW
Einstein-Hilbert
Curvature-squared contribution
Static warped geometries
Sound speed frequency dependence
SUPERLUMINALITY AND CAUSAL UV COMPLETIONS
Matter frame
M2PlTμν
Gravitationally induced matter interactions
Connection with the NEC
Positivity bounds for light fields
Scaling Limit
Light scalar fields
Electromagnetism
TT amplitude
Weakly coupled UV completion
Generic UV completion
Neglecting the t-channel pole
Higher derivative corrections
EFT matching
Curvature couplings to light fields
Subluminal spectator
Positivity bounds
EFFECTS FROM HIGHER-DIMENSION CURVATURE OPERATORS
One-loop effective action
Dimension-six curvature operators on FLRW
Modification of the dispersion relation
M2PlM2
M2PlM4
Dimension-eight curvature operators
DISCUSSION
Minimally coupled scalar field
Dimensional regularization
Full Text
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