Abstract

We present the first combination of NNLO QCD and NLO EW corrections for vector-boson pair production at the LHC. We consider all final states with two, three and four charged leptons, including resonant and non-resonant diagrams, spin correlations and off-shell effects. Detailed predictions are discussed for three representative channels corresponding to W+W−, W±Z and Z Z production. Both QCD and EW corrections are very significant, and the details of their combination can play a crucial role to achieve the level of precision demanded by experimental analyses. In this context we point out nontrivial issues that arise at large transverse momenta, where the EW corrections are strongly enhanced by Sudakov logarithms and the QCD corrections can feature so-called giant K -factors. Our calculations have been carried out in the Matrix+OpenLoops framework and can be extended to the production of an arbitrary colour singlet in hadronic collisions, provided that the required two-loop QCD amplitudes are available. Combined NNLO QCD and NLO EW predictions for the full set of massive diboson processes will be made publicly available in the next release of Matrix and will be instrumental in advancing precision diboson studies and new-physics searches at the LHC and future hadron colliders.

Highlights

  • The effect of the resummation of the large logarithmic terms at small transverse momenta up to next-to-next-to-leading logarithmic accuracy (NNLL) has been included in ref. [28]

  • We present the first combination of next-to-next-to-leading order (NNLO) QCD and NLO EW corrections for vector-boson pair production at the LHC

  • We present the first combination of NNLO QCD and NLO EW corrections for massive vector-boson pair production processes in their leptonic decay modes at the LHC

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Summary

Vector-boson pair production in NNLO QCD and NLO EW

The NNLO QCD and NLO EW computations for vector-boson pair production processes presented in this paper are carried out within the Matrix+OpenLoops framework. The required tree-level and one-loop amplitudes, including spin and colour correlations for the subtraction of infrared divergences, are calculated with OpenLoops 2 [52] This new version of the OpenLoops program supports the automated generation of matrix elements for any SM process at NLO QCD+NLO EW. For the calculation of off-shell vector-boson pair processes, 1Munich is the abbreviation of “MUlti-chaNnel Integrator at Swiss (CH) precision” — an automated parton-level NLO generator by S. The subtraction of IR singularities at NNLO is achieved through a fully general implementation of the qT -subtraction formalism [65] In this context, Matrix implements an automated extrapolation procedure to calculate integrated cross sections in the limit in which the cutoff parameter in the qT -subtraction procedure goes to zero [27]. The only restriction is given by the availability of the corresponding two-loop amplitudes

Overview of leptonic channels in vector-boson pair production
Higher-order QCD corrections
Higher-order EW corrections
Giant K-factors
Combination of QCD and EW corrections
Phenomenological results
Fiducial cross sections
Differential distributions without veto against QCD radiation
Results with a veto against hard QCD radiation
Summary and conclusions
Full Text
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