We calculate the complete electroweak O(α) corrections to p(-)p→l⁺l^-X(l=e,μ) in the standard model (SM) of electroweak interactions. They comprise weak and photonic virtual one-loop corrections as well as real photon radiation to the parton-level processes qq̄→γ,→Zl⁺l^-. We study in detail the effect of the radiative corrections on the l⁺l^- invariant mass distribution, the cross section in the Z boson resonance region, and on the forward-backward asymmetry AFB at the Fermilab Tevatron and the CERN Large Hadron Collider. The weak corrections are found to increase the Z boson cross section by about 1%, but have little effect on the forward-backward asymmetry in the Z peak region. Threshold effects of the W box diagrams lead to pronounced effects in AFB at m(l⁺l^-)≈160GeV which, however, will be difficult to observe experimentally. At high dilepton invariant masses, the nonfactorizable weak corrections are found to become large.
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Baur et al. (2002) studied this question.
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