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Next-to-leading order corrections to e+eW+WZ and e+eZZZ

Fawzi Boudjema, Le Duc Ninh, Sun Hao, and Marcus M. Weber
Phys. Rev. D 81, 073007 – Published 16 April 2010

Abstract

We calculate the one-loop electroweak corrections to e+eW+WZ and e+eZZZ and analyze their impacts on both the total cross section and some key distributions. These processes are important for the measurements of the quartic couplings of the massive gauge bosons which can be a window on the mechanism of spontaneous symmetry breaking. We find that even after subtracting the leading QED corrections, the electroweak corrections can still be large, especially as the energy increases. We compare and implement different methods of dealing with potential instabilities in the routines pertaining to the loop integrals. For the real corrections we apply a dipole subtraction formalism and compare it to a phase-space slicing method.

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  • Received 8 January 2010

DOI:https://doi.org/10.1103/PhysRevD.81.073007

©2010 American Physical Society

Authors & Affiliations

Fawzi Boudjema1, Le Duc Ninh2, Sun Hao1, and Marcus M. Weber2

  • 1Laboratoire d’Annecy-le-Vieux de Physique Théorique, Université de Savoie, CNRS, BP 110, F-74941 Annecy-le-Vieux Cedex, France
  • 2Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), D-80805 München, Germany

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Issue

Vol. 81, Iss. 7 — 1 April 2010

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Images

  • Figure 1
    Figure 1
    Representative Born diagrams for e+eZZZ and e+eW+WZ. Diagrams (a) contribute to both processes while diagrams of type (b) contribute only to e+eW+WZ. The first diagram of type (a) will be referred to as the Higgsstrahlung contribution.Reuse & Permissions
  • Figure 2
    Figure 2
    Dependence of σreale+eW+WZγ on the soft cutoff δs in phase-space slicing with fixed δc=7·104. Only the nonsingular part is shown, i.e. the IR singular ln(mγ2) terms are set to zero. The result using dipole subtraction is shown for comparison with the error given by the width of the band.Reuse & Permissions
  • Figure 3
    Figure 3
    Left: the total cross section for e+eZZZ as a function of s for the Born, full O(α), and genuine weak correction for MH=120GeV. Right: the corresponding relative percentage corrections σNLO/σLO1.Reuse & Permissions
  • Figure 4
    Figure 4
    From top to bottom: distributions for the ZZ invariant mass, the rapidity of the Z and the transverse momentum of the Z for e+eZZZ at s=500GeV and MH=120GeV. The panels on the left show the tree level, the full NLO, and the weak correction. The panels on the right show the corresponding relative (to the tree level) percentage corrections. The distributions are obtained by entering for each event the corresponding observable, say pTZ, of each Z and then normalizing by a factor 1/3.Reuse & Permissions
  • Figure 5
    Figure 5
    Left: the total cross section for e+eW+WZ as a function of s for the Born, full O(α), and genuine weak correction for MH=120GeV. Right: the corresponding relative percentage corrections σNLO/σLO1.Reuse & Permissions
  • Figure 6
    Figure 6
    From top to bottom: distributions for the WW invariant mass, the rapidity of the WW system and the transverse momentum of the Z for e+eW+WZ at s=500GeV and MH=120GeV. The panels on the left show the tree level, the full NLO, and the weak correction. The panels on the right show the corresponding relative (to the tree level) percentage corrections.Reuse & Permissions
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