2008
DOI: 10.1103/physrevd.77.025018
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New dual conformally invariant off-shell integrals

Abstract: Evidence has recently emerged for a hidden symmetry of planar scattering amplitudes in N 4 superYang-Mills theory called dual conformal symmetry. At weak coupling the presence of this symmetry has been observed through five loops, while at strong coupling the symmetry has been shown to have a natural interpretation in terms of a T-dualized AdS 5 . In this paper we study dual conformally invariant off-shell four-point Feynman diagrams. We classify all such diagrams through four loops and evaluate 10 new offshel… Show more

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Cited by 35 publications
(27 citation statements)
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“…Secondly, the gluon amplitudes have the intriguing property of 'dual' conformal symmetry [25] (see also [9,44]). All the scalar Feynman integrals appearing in the calculations of Bern et al up to four loops 20 are dual to conformal integrals, after we take them off shell and perform the change of variables (6) from momenta to 'dual coordinates'.…”
Section: Discussionmentioning
confidence: 99%
“…Secondly, the gluon amplitudes have the intriguing property of 'dual' conformal symmetry [25] (see also [9,44]). All the scalar Feynman integrals appearing in the calculations of Bern et al up to four loops 20 are dual to conformal integrals, after we take them off shell and perform the change of variables (6) from momenta to 'dual coordinates'.…”
Section: Discussionmentioning
confidence: 99%
“…Similar representations can be derived also for the 4-point functions, (see e.g. [10] for the case L = 3). Let us stress that, although all the propagators are massless, since in general x 2 ij = 0, one has to compute these "momentum space like" integrals with off-shell external legs.…”
Section: Alternative Representations Of G Lmentioning
confidence: 86%
“…(12) has been considered, in a particular kinematical regime appropriate for taking the on-shell limit, in [10] where also a MellinBarnes representation has been derived. Before proceeding to the proof in the case of general L, we list the expressions for the simpler cases of L = 1 …”
Section: Introductionmentioning
confidence: 99%
“…The divergent part of the integral over y 1 is thus 18) and the remaining integral over y 2 diverges whenever λ j (y 2 ) = λ k (y 2 ), i.e., when y 2 is a root of the discriminant discrim y 1 (G). It is also clear that these roots are the angles of our boundary G(y 1 , y 2 ) = 0, which consists of lines y 1 = λ i (y 2 ) that form angles at intersection points, and these angles produce quadratic divergencies.…”
Section: Methods Of Proceeding In ε-Regularizationmentioning
confidence: 99%