A generalized leading-term approximation of high-energy scattering amplitudes in Yang-Mills theory

1979 ◽  
Vol 157 (2) ◽  
pp. 212-236 ◽  
Author(s):  
C.Y. Lo
1979 ◽  
Vol 25 (6) ◽  
pp. 175-181 ◽  
Author(s):  
H. Cheng ◽  
J. Dickinson ◽  
C. Y. Lo ◽  
K. Olaussen

1981 ◽  
Vol 23 (2) ◽  
pp. 534-552 ◽  
Author(s):  
Hung Cheng ◽  
John A. Dickinson ◽  
Kaare Olaussen

1967 ◽  
Vol 160 (5) ◽  
pp. 1296-1305 ◽  
Author(s):  
A. H. Mueller ◽  
T. L. Trueman

2014 ◽  
Vol 29 (27) ◽  
pp. 1450154 ◽  
Author(s):  
Georgios Papathanasiou

The simplicity of maximally supersymmetric Yang–Mills theory makes it an ideal theoretical laboratory for developing computational tools, which eventually find their way to QCD applications. In this contribution, we continue the investigation of a recent proposal by Basso, Sever and Vieira, for the nonperturbative description of its planar scattering amplitudes, as an expansion around collinear kinematics. The method of G. Papathanasiou, J. High Energy Phys.1311, 150 (2013), arXiv:1310.5735, for computing the integrals the latter proposal predicts for the leading term in the expansion of the six-point remainder function, is extended to one of the subleading terms. In particular, we focus on the contribution of the two-gluon bound state in the dual flux tube picture, proving its general form at any order in the coupling, and providing explicit expressions up to six loops. These are included in the ancillary file accompanying the version of this paper on the arXiv.


Sign in / Sign up

Export Citation Format

Share Document