Abstract
We compute the one-loop scalar massless pentagon integral I 6−2ϵ5 in D = 6−2ϵ dimensions in the limit of multi-Regge kinematics. This integral first contributes to the parity-odd part of the one-loop \( \mathcal{N} \) = 4 five-point MHV amplitude m (1)5 at \( \mathcal{O} \)(ϵ). In the high energy limit defined by s ≫ s 1, s 2 ≫ −t 1,−t 2, the pentagon integral reduces to double sums or equivalently twofold Mellin-Barnes integrals. By determining the \( \mathcal{O} \)(ϵ) contribution to I 6−2ϵ5 , one therefore gains knowledge of m (1)5 to \( \mathcal{O} \)(ϵ2) which is necessary for studies of the iterative structure of \( \mathcal{N} \) = 4 SYM amplitudes beyond one-loop. One immediate application is the extraction of the one-loop gluon-production vertex to \( \mathcal{O} \)(ϵ2) and the iterative construction of the two-loop gluon-production vertex including finite terms which is described in a companion paper [1]. The analytic methods we have used for evaluating the one-loop pentagon integral in the high energy limit may also be applied to the hexagon integral and may ultimately give information on the form of the R (2)6 remainder function.
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ArXiv ePrint: 0905.0097
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Del Duca, V., Duhr, C., Nigel Glover, E.W. et al. The one-loop pentagon to higher orders in ϵ. J. High Energ. Phys. 2010, 42 (2010). https://doi.org/10.1007/JHEP01(2010)042
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DOI: https://doi.org/10.1007/JHEP01(2010)042