Abstract

We present the analytic calculation of the Master Integrals necessary to compute the planar massive QCD corrections to Di-photon (and Di-jet) production at hadron colliders. The master integrals are evaluated by means of the differential equations method and expressed in terms of multiple polylogarithms and one- or two-fold integrals of polylogarithms and irrational functions, up to transcendentality four.

Highlights

  • We present the analytic calculation of the Master Integrals necessary to compute the planar massive QCD corrections to Di-photon production at hadron colliders

  • In this article we presented the calculation of the master integrals needed for the evaluation of the NNLO QCD planar corrections to di-photon production in hadronic collisions

  • We represented these integrals in terms of Goncharov’s multiple polylogarithms (GPLs), whenever it was possible to linearize the set of square roots appearing in the corresponding alphabet

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Summary

Notations

We consider the basic processes qq → γγ, (gg, qq) and the crossed q(q)g → q(q)g, in which the initial partons have momenta p1 and p2 and the final photons or partons have momenta p3 and p4. Since we consider 2 → 2 scattering processes with massless external particles, the physical region is defined through the following relations s s > 0 , t = − (1 − cos θ) < 0 , −s < t < 0 ,. The NNLO QCD planar corrections to the partonic processes listed above can be calculated reducing to the MIs two topologies, shown in figure 1 and defined by the integrals. There are three-point functions that are not included in the subtopologies of topologies A and B These are the three-point functions that occur for instance in the calculation of the NLO QCD corrections to the Higgs production in gluon fusion (or Higgs decay into a pair of photons) and the corresponding MIs were studied in [39, 40]

The system of differential equations
The master integrals
Conclusions
A Linearization of square roots
B Routing for the pre-canonical master integrals
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