Abstract
Wilson loops with lightlike polygonal contours have been conjectured to be equivalent to MHV scattering amplitudes in \( \mathcal{N} \) = 4 super Yang-Mills. We compute such Wilson loops for special polygonal contours at two loops in perturbation theory. Specifically, we concentrate on the remainder function \( \mathcal{R} \), obtained by subtracting the known ABDK/BDS ansatz from the Wilson loop. First, we consider a particular two dimensional eight-point kinematics studied at strong coupling by Alday and Maldacena. We find numerical evidence that \( \mathcal{R} \) is the same at weak and at strong coupling, up to an overall, coupling-dependent constant. This suggests a universality of the remainder function at strong and weak coupling for generic null polygonal Wilson loops, and therefore for arbitrary MHV amplitudes in \( \mathcal{N} \) = 4 super Yang-Mills. We analyse the consequences of this statement. We further consider regular n-gons, and find that the remainder function is linear in n at large n through numerical computations performed up to n = 30. This reproduces a general feature of the corresponding strong-coupling result.
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ArXiv ePrint: 0910.4898
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Brandhuber, A., Heslop, P., Khoze, V.V. et al. Simplicity of polygon Wilson loops in \( \mathcal{N} \) = 4 SYM. J. High Energ. Phys. 2010, 50 (2010). https://doi.org/10.1007/JHEP01(2010)050
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DOI: https://doi.org/10.1007/JHEP01(2010)050