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A bstract Radiative corrections in pole approximation, which are based on the leading contribution in a systematic expansion of amplitudes about resonance poles, naturally decompose into factorizable corrections attributed to the production or decay of the resonance and non-factorizable corrections induced by soft photon (or gluon) exchange between those subprocesses. In this paper we complete an earlier calculation of mixed QCD × electroweak corrections of O (ₒ) to the neutral-current Drell-Yan cross section in pole approximation by including the previously neglected corrections that are solely related to the Z-boson production process. We present numerical results both for differential distributions and for the forward-backward asymmetry differential in the lepton-pair invariant mass, which is the key observable in the measurement of the effective weak mixing angle at the LHC. Carefully disentangling the various types of factorizable and non-factorizable corrections, we find (as expected in our earlier work) that the by far most important contribution at O (ₒ) originates from the interplay of initial-state QCD corrections and electroweak final-state corrections.
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Stefan Dittmaier
University of Vienna
Alexander Huss
European Organization for Nuclear Research
Jan Schwarz
University of Freiburg
Journal of High Energy Physics
University of Freiburg
European Organization for Nuclear Research
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Dittmaier et al. (Tue,) studied this question.
synapsesocial.com/papers/68e6a293b6db6435876265fc — DOI: https://doi.org/10.1007/jhep05(2024)170
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