Abstract
The numerical evaluation of multi-loop scattering amplitudes in the Feynman representation usually requires to deal with both physical (causal) and unphysical (non-causal) singularities. The loop-tree duality (LTD) offers a powerful framework to easily characterise and distinguish these two types of singularities, and then simplify analytically the underling expressions. In this paper, we work explicitly on the dual representation of multi-loop Feynman integrals generated from three parent topologies, which we refer to as Maximal, Next-to-Maximal and Next-to-Next-to-Maximal loop topologies. In particular, we aim at expressing these dual contributions, independently of the number of loops and internal configurations, in terms of causal propagators only. Thus, providing very compact and causal integrand representations to all orders. In order to do so, we reconstruct their analytic expressions from numerical evaluation over finite fields. This procedure implicitly cancels out all unphysical singularities. We also interpret the result in terms of entangled causal thresholds. In view of the simple structure of the dual expressions, we integrate them numerically up to four loops in integer space-time dimensions, taking advantage of their smooth behaviour at integrand level.
Highlights
The numerical evaluation of multi-loop scattering amplitudes in the Feynman representation usually requires to deal with both physical and unphysical singularities
In former works [19], we have demonstrated how the loop-tree duality (LTD) formalism provides a comprehensive classification of causal singularities and how unphysical ones are cancelled among paired terms
We have explicitly elaborated on the analytical structure of the Maximal (MLT), Next-to-Maximal (NMLT) and Next-to-Next-to-Maximal (N2MLT) loop topologies to all orders
Summary
We set the notation and review the main features of the loop-tree duality (LTD) formalism. We have explicitly pulled out in eq (2.3) the dependence of the Feynman propagator on the energy component of the loop momentum because we will integrate out this component explicitly. Since all the propagators are written in terms of independent loop momenta, we classify them through the flowing between them. In order to obtain the LTD representation for a given scattering amplitude, it is necessary to apply the Cauchy residue theorem iteratively and integrate out one degree of freedom for each loop momentum. Starting from eq (2.1) and setting on shell the propagators that depend on the first loop momentum, qi, we define,. The final LTD representation is given by the sum of all the nested residues and corresponds to setting simultaneously L lines on shell, which is equivalent to open the loop amplitude to non-disjoint trees.
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