Abstract

Gravitational waves (GW), as light, are gravitationally lensed by intervening matter, deflecting their trajectories, delaying their arrival and occasionally producing multiple images. In theories beyond general relativity (GR), new gravitational degrees of freedom add an extra layer of complexity and richness to GW lensing. We develop a formalism to compute GW propagation beyond GR over general space-times, including kinetic interactions with new fields. Our framework relies on identifying the dynamical propagation eigenstates (linear combinations of the metric and additional fields) at leading order in a short-wave expansion. We determine these eigenstates and the conditions under which they acquire a different propagation speed around a lens. Differences in speed between eigenstates cause birefringence phenomena, including time delays between the metric polarizations (orthogonal superpositions of $h_+,h_\times$) observable without an electromagnetic counterpart. In particular, GW echoes are produced when the accumulated delay is larger than the signal's duration, while shorter time delays produce a scrambling of the wave-form. We also describe the formation of GW shadows as non-propagating metric components are sourced by the background of the additional fields around the lens. As an example, we apply our methodology to quartic Horndeski theories with Vainshtein screening and show that birefringence effects probe a region of the parameter space complementary to the constraints from the multi-messenger event GW170817. In the future, identified strongly lensed GWs and binary black holes merging near dense environments, such as active galactic nuclei, will fulfill the potential of these novel tests of gravity.

Highlights

  • The detection of gravitational wave (GW) signals from black-hole and neutron-star mergers provides a direct probe of Einstein’s general relativity (GR) and fundamental properties of gravity

  • For any given gravity theory, the propagation of GWs can be determined from the equations of motion (EOM) for the linearized perturbations, which are obtained expanding around the background metric gtμoνt 1⁄4 gμν þ hμν: ð1Þ

  • There are four signals whose propagation can be studied at leading order in GW lensing beyond GR: electromagnetic radiation traveling at speed c0 ≡ c and three propagation eigenstates traveling at speeds c1, c2, c3, which depend on the interaction basis speeds ch, cs, cm and the mixing Mφ

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Summary

INTRODUCTION

The detection of gravitational wave (GW) signals from black-hole and neutron-star mergers provides a direct probe of Einstein’s general relativity (GR) and fundamental properties of gravity These tests have far reaching implications for cosmology, probing the accelerated expansion of the universe and dark energy models in a manner complementary to “traditional” observations based on electromagnetic (EM) radiation [1]. (3) beyond FRW effects can introduce new scales and affect the gravitational polarizations (þ; ×) differently, providing signatures that do not require an electromagnetic (EM) counterpart This enables tests from black hole (BH) binaries, applicable to more events and at higher redshift. As we will discuss here, theories beyond GR extend the range of gravitational lensing phenomena even further

Summary for the busy reader
THE PROBLEM: A GENERAL THEORY FOR GRAVITATIONAL RADIATION
Gauge fixing
Identifying the radiative degrees of freedom
Short-wave approximation
GW LENSING BEYOND GENERAL RELATIVITY
Propagation eigenstates
Deflection angle
Time delays
Observational regimes: scrambling and echoes
Single lens
Multiple lenses
Source near the lens
Strong vs weak lensing and multiple images
Lensing probabilities
PROPAGATION EIGENSTATES IN HORNDESKI THEORIES
Luminal theories
Generalized Brans-Dicke
Kinetic gravity braiding
Luminal Horndeski gravity
Nonluminal theories
Quartic theories
Quintic theories
PROBING GW PROPAGATION IN SCREENED REGIONS
Local background
Cosmological background
Shapiro time delay
Geometrical time delay
Multiple image time delays
Polarization mixing and GW shadows
Observational prospects
CONCLUSIONS AND PROSPECTS
CA ðDφφÞ φ
Shift-symmetric quartic Horndeski
Full Text
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