High-energy massless gravitational scattering in N = 8 supergravity was recently analyzed at leading level in the deflection angle, uncovering an interesting connection between exponentiation of infrared divergences in momentum space and the eikonal exponentiation in impact parameter space. Here we extend that analysis to the first non trivial sub-leading level in the deflection angle which, for massless external particles, implies going to two loops, i.e. to third post-Minkowskian (3PM) order. As in the case of the leading eikonal, we see that the factorisation of the momentum space amplitude into the exponential of the one-loop result times a finite remainder hides some basic simplicity of the impact parameter formulation. For the conserv...
Using N = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for t...
Abstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM ...
Radiation reaction (RR) terms at the third post-Minkowskian (3PM) order have recently been found to ...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
High-energy massless gravitational scattering in N = 8 supergravity was recently analyzed at leading...
High-energy massless gravitational scattering in ${\cal N}=8$ supergravity was recently analyzed at ...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
The aim of this article is to explore the interplay between the eikonal resummation in impact-parame...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
Following a semiclassical eikonal approach—justified at transplanckian energies order by order in th...
Using soft-graviton theorems a well-known zero-frequency limit (ZFL) for the gravitational radiation...
Using $ \mathcal{N} $ = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational...
We derive an ABDK-like relation between the one- and two-loop four-graviton amplitudes in N = 8 supe...
Using N = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for t...
Abstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM ...
Radiation reaction (RR) terms at the third post-Minkowskian (3PM) order have recently been found to ...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
High-energy massless gravitational scattering in N = 8 supergravity was recently analyzed at leading...
High-energy massless gravitational scattering in ${\cal N}=8$ supergravity was recently analyzed at ...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
The aim of this article is to explore the interplay between the eikonal resummation in impact-parame...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
Following a semiclassical eikonal approach—justified at transplanckian energies order by order in th...
Using soft-graviton theorems a well-known zero-frequency limit (ZFL) for the gravitational radiation...
Using $ \mathcal{N} $ = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational...
We derive an ABDK-like relation between the one- and two-loop four-graviton amplitudes in N = 8 supe...
Using N = 8 supergravity as a theoretical laboratory, we extract the 3PM gravitational eikonal for t...
Abstract Using N $$ \mathcal{N} $$ = 8 supergravity as a theoretical laboratory, we extract the 3PM ...
Radiation reaction (RR) terms at the third post-Minkowskian (3PM) order have recently been found to ...