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L. F. Alday, J. M. Maldacena, “Gluon scattering amplitudes at strong coupling,” JHEP 0706
Original
2007
Earlier work this paper cites.
L. F. Alday and J. M. Maldacena, “Comments on operators with large spin,” JHEP 0711
Original
2007
Earlier work this paper cites.
G. P. Korchemsky, J. M. Drummond, E. Sokatchev, “Conformal properties of four-gluon planar amplitudes and Wilson loops,” Nucl. Phys. B795
Original
2008
Earlier work this paper cites.
A. Brandhuber, P. Heslop and G. Travaglini, “A Note on dual superconformal symmetry of the N=4 super Yang-Mills S-matrix,” Phys. Rev. D 78
Original
2008
Earlier work this paper cites.
J. M. Drummond, J. Henn, G. P. Korchemsky and E. Sokatchev, “Dual superconformal symmetry of scattering amplitudes in N=4 super-Yang-Mills theory,” Nucl. Phys. B 828
Original
2009
Earlier work this paper cites.
J. M. Drummond and J. M. Henn, “All tree-level amplitudes in N=4 SYM,” JHEP 0904
Original
2009
Earlier work this paper cites.
H. Elvang, D. Z. Freedman and M. Kiermaier, “Solution to the Ward Identities for Superamplitudes,” JHEP 1010
Original
2010
Earlier work this paper cites.

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2011
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Original

Then

B. Basso, A. Sever and P. Vieira, “Space-time S-matrix and Flux-tube S-matrix IV. Gluons and Fusion,” JHEP 1409
Original
2014
Later among the works it cites.
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Original
2015
Later among the works it cites.
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Original
2015
Later among the works it cites.
B. Basso, J. Caetano, L. Cordova, A. Sever and P. Vieira, “OPE for all Helicity Amplitudes II. Form Factors and Data analysis,” JHEP 1512
Original
2015
Later among the works it cites.
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2016

Hexagon POPE: effective particles and tree level resummation

Córdova, Lucía

Understand

We present the resummation of the full Pentagon Operator Product Expansion series of the hexagon Wilson loop in planar $\mathcal N=4$ SYM at tree level.

We do so by considering the one effective particle states formed by a fundamental flux tube excitation and an arbitrary number of the so called "small fermions" which are then integrated out.
We present our proposals for the one effective particle measures at finite coupling.
By evaluating these measures at tree level and summing over all one effective particle states we reproduce the full 6 point tree level amplitude.