The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3)
Abstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for two colliding massive scalars from the classical limit of the corresponding elastic two-loop amplitude. We employ the eikonal phase to obtain the physical deflection angle an...
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Online Access: | https://doi.org/10.1007/JHEP07(2021)169 |
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doaj-17a68a981bbc43e5bb4e60173e42e5212021-07-25T11:45:23ZengSpringerOpenJournal of High Energy Physics1029-84792021-07-012021718010.1007/JHEP07(2021)169The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3)Paolo Di Vecchia0Carlo Heissenberg1Rodolfo Russo2Gabriele Veneziano3The Niels Bohr Institute, University of CopenhagenNORDITA, KTH Royal Institute of Technology and Stockholm UniversityCentre for Research in String Theory, School of Physics and Astronomy, Queen Mary University of LondonTheory Department, CERNAbstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for two colliding massive scalars from the classical limit of the corresponding elastic two-loop amplitude. We employ the eikonal phase to obtain the physical deflection angle and to show how its non-relativistic (NR) and ultra-relativistic (UR) regimes are smoothly connected. Such a smooth interpolation rests on keeping contributions to the loop integrals originating from the full soft region, rather than restricting it to its potential sub-region. This task is efficiently carried out by using the method of differential equations with complete near-static boundary conditions. In contrast to the potential-region result, the physical deflection angle includes radiation-reaction contributions that are essential for recovering the finite and universal UR limit implied by general analyticity and crossing arguments. We finally discuss the real emission of massless states, which accounts for the imaginary part of the 3PM eikonal and for the dissipation of energy-momentum. Adopting a direct approach based on unitarity and on the classical limit of the inelastic tree-level amplitude, we are able to treat N $$ \mathcal{N} $$ = 8 and General Relativity on the same footing, and to complete the conservative 3PM eikonal in Einstein’s gravity by the addition of the radiation-reaction contribution. We also show how this approach can be used to compute waveforms, as well as the differential and integrated spectra, for the different radiated massless fields.https://doi.org/10.1007/JHEP07(2021)169Black HolesClassical Theories of GravityScattering AmplitudesSupergravity Models |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Paolo Di Vecchia Carlo Heissenberg Rodolfo Russo Gabriele Veneziano |
spellingShingle |
Paolo Di Vecchia Carlo Heissenberg Rodolfo Russo Gabriele Veneziano The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) Journal of High Energy Physics Black Holes Classical Theories of Gravity Scattering Amplitudes Supergravity Models |
author_facet |
Paolo Di Vecchia Carlo Heissenberg Rodolfo Russo Gabriele Veneziano |
author_sort |
Paolo Di Vecchia |
title |
The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) |
title_short |
The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) |
title_full |
The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) |
title_fullStr |
The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) |
title_full_unstemmed |
The eikonal approach to gravitational scattering and radiation at O $$ \mathcal{O} $$ (G 3) |
title_sort |
eikonal approach to gravitational scattering and radiation at o $$ \mathcal{o} $$ (g 3) |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2021-07-01 |
description |
Abstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for two colliding massive scalars from the classical limit of the corresponding elastic two-loop amplitude. We employ the eikonal phase to obtain the physical deflection angle and to show how its non-relativistic (NR) and ultra-relativistic (UR) regimes are smoothly connected. Such a smooth interpolation rests on keeping contributions to the loop integrals originating from the full soft region, rather than restricting it to its potential sub-region. This task is efficiently carried out by using the method of differential equations with complete near-static boundary conditions. In contrast to the potential-region result, the physical deflection angle includes radiation-reaction contributions that are essential for recovering the finite and universal UR limit implied by general analyticity and crossing arguments. We finally discuss the real emission of massless states, which accounts for the imaginary part of the 3PM eikonal and for the dissipation of energy-momentum. Adopting a direct approach based on unitarity and on the classical limit of the inelastic tree-level amplitude, we are able to treat N $$ \mathcal{N} $$ = 8 and General Relativity on the same footing, and to complete the conservative 3PM eikonal in Einstein’s gravity by the addition of the radiation-reaction contribution. We also show how this approach can be used to compute waveforms, as well as the differential and integrated spectra, for the different radiated massless fields. |
topic |
Black Holes Classical Theories of Gravity Scattering Amplitudes Supergravity Models |
url |
https://doi.org/10.1007/JHEP07(2021)169 |
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