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The electroweak O(α) contribution to the resonant single W production in a general four-fermion process is discussed with particular emphasis on a gauge-invariant decomposition into a QED-like and weak part. The cross section in the vicinity of the resonance can be represented in terms of a convolution of a ``hard'' Breit-Wigner cross section, comprising the (mₜ,MH)-dependent weak one-loop corrections, with a universal radiator function. The numerical impact of the various contributions on the W line shape are discussed, together with the concepts of s-dependent and constant width approaches. Analytic formulas for the W decay width are also provided including the one-loop electroweak and QCD corrections.
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Wackeroth et al. (1997) studied this question.
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