Abstract

We explore a direct connection between the collinear limit and the multi-Regge limit for scattering amplitudes in the $$ \mathcal{N} $$ = 4 super Yang-Mills theory. Starting with the collinear expansion for the six-gluon amplitude in the Euclidean kinematic region, we perform an analytic continuation term by term to the so-called Mandelstam region. We find that the result coincides with the collinear expansion of the analytically continued amplitude. We then take the multi-Regge limit, and conjecture that the final result precisely reproduces the one from the BFKL approach. Combining this procedure with the OPE for null polygonal Wilson loops, we explicitly compute the leading contribution in the “collinear-Regge” limit up to five loops. Our results agree with all the known results up to four loops. At five-loop, our results up to the next-to-next-to-leading logarithmic approximation (NNLLA) also reproduce the known results, and for the N3LLA and the N4LLA give non-trivial predictions. We further present an all-loop prediction for the imaginary part of the next-to-double-leading logarithmic approximation. Our procedure has a possibility of an interpolation from weak to strong coupling in the multi-Regge limit with the help of the OPE.

Highlights

  • One of the most remarkable feature for the scattering amplitude in the N = 4 SYM is that it has a hidden symmetry in momentum space, called dual conformal symmetry [5, 6]

  • We found a direct connection between the collinear limit in the Euclidean region and the multi-Regge limit in the Mandelstam region

  • The former is systematically treated by the Wilson loop operator product expansion (OPE) while the latter by the BFKL approach

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Summary

Collinear limit and multi-Regge limit

Let us start by reviewing the collinear limit and the multi-Regge limit. Introducing the momentum invariants by si...j = (pi + · · · + pj), the multi-Regge limit is defined by the following scale hierarchy s12 ≫ s345, s456 ≫ s34, s45, s56 ≫ s23, s61, s234. This limit is shown in figure 1(a). The cross-ratios are expressed by the momentum invariants as follows, s12 s234. In the multi-Regge limit, the three cross-ratios behave as (u1, u2, u3) → (0, 0, 1).

Analytic continuation from Euclidean to Mandelstam region
BFKL approach
Two-loop analysis
Collinear limit of two-loop remainder function
Analytic continuation and collinear limit
Collinear-Regge expansion
Higher loops and Wilson loop OPE
Three-loop analysis
Wilson loop OPE
Higher-loop results
Double-leading-logarithmic approximation and beyond
Two-particle contributions in OPE
Comment on analytic continuation at finite coupling
Conclusions
A Analytic continuation of two-loop remainder function
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