Abstract

We derive the classical gravitational radiation from an aligned spin binary black hole on closed orbits, using a dictionary built from the 5-point QFT scattering amplitude of two massive particles exchanging and emitting a graviton. We show explicitly the agreement of the transverse-traceless components of the radiative linear metric perturbations — and the corresponding gravitational wave energy flux — at future null infinity, derived from the scattering amplitude and those derived utilizing an effective worldline action in conjunction with multipolar post-Minkowskian matching. At the tree-level, this result holds at leading orders in the black holes’ velocities and up to quadratic order in their spins. At sub-leading order in black holes’ velocities, we demonstrate a matching of the radiation field for quasi-circular orbits in the no-spin limit. At the level of the radiation field, and to leading order in the velocities, there exists a one-to-one correspondence between the binary black hole mass and current quadrupole moments, and the scalar and linear-in-spin scattering amplitudes, respectively. Therefore, we show explicitly that waveforms, needed to detect gravitational waves from inspiraling binary black holes, can be derived consistently, to the orders considered, from the classical limit of quantum scattering amplitudes.

Highlights

  • Until recently, the scattering amplitudes approach to the two-body scattering problem had mostly focused it’s efforts in the conservative sector, hints from soft theorems suggest that they can be used to address the radiative sector [47,48,49]

  • In this work we follow this philosophy to compute the gravitational waveform emitted from an aligned spin BBH on general and quasi-circular orbits, up to quadratic order in the constituents spin at the leading order in the velocity expansion and to sub-leading order in the no-spin limit, from a 5-pt scattering amplitude of two massive particles exchanging and emitted gravitons

  • At quadratic order in the black hole (BH)’ spins, and for quasi-circular orbits, we demonstrate that the contribution from the quadratic in spin amplitude is canceled by the contribution of the scalar amplitude in conjunction with the O(S2)-piece of the equations of motion (EoM) (2.5)

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Summary

Classical derivation

In order to approach the bound orbit from a classical point of view, we utilize an effective worldline action [12, 75,76,77,78,79,80], parametrizing the complete set of spin-induced interactions of the two spinning BHs in the weak-field regime, at linear order in the gravitational constant, i.e. at PM order. [79, 81,82,83,84,85,86,87,88,89,90,91,92,93,94] Using these results, we tackle the radiative sector, utilizing the multipolar post-Minkowskian formalism [4, 71,72,73,74]

Classical spinning binary black hole
Effective binary black hole action
Conservative dynamics
Linearized metric perturbations at null infinity
General approach
Gravitational radiation from spinning binary black hole
Scattering amplitudes derivation
Scattering amplitude and double copy
Electromagnetic 5-pt amplitude
Gravitational 5-pt amplitude
Computation of the radiated field
Scalar waveform
Linear-in-spin waveform
Cancellations at quadratic order in spin
Scalar waveform at sub-leading order in velocities
Radiated gravitational wave energy flux
Discussion
A Useful integrals and identities
B The quadratic in spin EoM
Full Text
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