2019
DOI: 10.1103/physrevd.100.124007
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Polarization modes of gravitational waves in quadratic gravity

Abstract: The observation of the inspiral and merger of compact binaries by the LIGO-Virgo collaboration has allowed for new tests of Einstein's theory in the extreme gravity regime, where gravitational interactions are simultaneously strong, non-linear, and dynamical. Theories beyond Einstein's can also be constrained by detecting the polarization modes of gravitational waves. In this paper, we show that dynamical Chern-Simons and Einstein-dilaton-Gauss-Bonnet gravity cannot be differentiated from general relativity ba… Show more

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Cited by 31 publications
(23 citation statements)
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“…In certain modified theories, a graviton can propagate with up to six polarizations, thereby leaving no residual gauge freedom. However, for the case of dCS gravity, GWs continue to propagate with only two polarizations (as measured at future null infinity) [54,55], and thus, one retains enough gauge freedom to impose the Regge-Wheeler gauge. Such a decomposition separates the axial and polar perturbations with different harmonic index ℓ, i.e., for a given ℓ, we have two systems of evolution equations, one for the axial sector and one for the polar sector.…”
Section: Black Hole Perturbation Theory a Decomposition Of The Fundam...mentioning
confidence: 99%
“…In certain modified theories, a graviton can propagate with up to six polarizations, thereby leaving no residual gauge freedom. However, for the case of dCS gravity, GWs continue to propagate with only two polarizations (as measured at future null infinity) [54,55], and thus, one retains enough gauge freedom to impose the Regge-Wheeler gauge. Such a decomposition separates the axial and polar perturbations with different harmonic index ℓ, i.e., for a given ℓ, we have two systems of evolution equations, one for the axial sector and one for the polar sector.…”
Section: Black Hole Perturbation Theory a Decomposition Of The Fundam...mentioning
confidence: 99%
“…where A ψ and A µ are the amplitudes, while k µ andk ν represent the wave-vcectors. From Equations (23), (26), and (28), one also concludes that the transverse-traceless part h µν , vector perturbation φ (1)µ , and scalar perturbation ψ propogate at the speed of light [54].…”
Section: Linearized Field Equationsmentioning
confidence: 88%
“…Since the resultant SET is averaged, one may utilize the integration by parts to eliminate the boundary terms. Furthermore, by plugging in the equation of motion of the first order perturbations, Equations (23), (26), and (28), while imposing the transverse-traceless gauge for h µν , one finds (50) In particular, if the vector (φ µ ) and scalar (µ) fields vanish, it is readily to show that the action Equation (2) falls back to the Brans-Dicke theory by redefiningφ = 1/G. Also, the result given by Equation 50is consistent with the GW SET of Brans-Dicke theory in [39,62].…”
Section: The Stress-energy Pseudo-tensormentioning
confidence: 99%
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“…We have known the polarization modes of gravitational waves predicted by some modified gravities, like Brans-Dicke, f (R), Horndeski, Einstein-ather, TeVeS, Horava, STVG, f (T ), dCS and EdGB theory [6,[14][15][16][17][18][19][20]. In these studies, the Newman-Penrose formalism was often used in the case of plane gravitational waves propagating at the speed of light [6,21].…”
Section: Introductionmentioning
confidence: 99%