We derive an ABDK-like relation between the one- and two-loop four-graviton amplitudes in N = 8 supergravity. Specifically we show that the infrared-divergent part of the two-loop amplitude is one-half the square of the one-loop amplitude, suggesting an exponential structure for IR divergences. The difference between the two-loop amplitude and one-half the square of the full one-loop amplitude is therefore finite, and expressible in a relatively simple form. We give arguments for generalizations to higher loops and n-point functions, suggesting that the exponential of the full one-loop amplitude may be corrected, to low orders, by only simple finite terms. © 2008 Elsevier B.V. All rights reserved
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
We apply factorization and eikonal methods from gauge theories to scattering amplitudes in gravity. ...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
We present the full two-loop four-graviton amplitudes in N = 4, 5, 6 supergravity. These results wer...
The infrared singularities of gravitational amplitudes are one-loop exact, in that higher-loop diver...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
International audienceThe structure of scattering amplitudes in supergravity theories continues to b...
The infrared singularities of gravitational amplitudes are one-loop exact, in that higher-loop diver...
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Abstract We compute the three-loop scattering amplitude of fou...
We examine in detail the structure of the Regge limit of the (nonplanar) N = 4 SYM four-point amplit...
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 ...
AbstractWe present compact formulas for the box coefficients of the six-graviton NMHV one-loop ampli...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
We apply factorization and eikonal methods from gauge theories to scattering amplitudes in gravity. ...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
We present the full two-loop four-graviton amplitudes in N = 4, 5, 6 supergravity. These results wer...
The infrared singularities of gravitational amplitudes are one-loop exact, in that higher-loop diver...
The structure of scattering amplitudes in supergravity theories continues to be of interest. Recentl...
International audienceThe structure of scattering amplitudes in supergravity theories continues to b...
The infrared singularities of gravitational amplitudes are one-loop exact, in that higher-loop diver...
Abstract We compute the three-loop scattering amplitude of four gravitons in N = 8 $$ \mathcal{N}=8 ...
Abstract We compute the three-loop scattering amplitude of fou...
We examine in detail the structure of the Regge limit of the (nonplanar) N = 4 SYM four-point amplit...
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 ...
AbstractWe present compact formulas for the box coefficients of the six-graviton NMHV one-loop ampli...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
High-energy massless gravitational scattering in $ \mathcal{N} $ = 8 supergravity was recently analy...
We apply factorization and eikonal methods from gauge theories to scattering amplitudes in gravity. ...