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Non-factorizable photonic corrections to ee->WW->4fermions

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arxiv hep-ph/9710521 v3 pith:YR4WCRSY submitted 1997-10-29 hep-ph

classification hep-ph
keywords correctionsnon-factorizableanalyticaldistributionfullnumericalparametrizationproduction
verification ladder T0 review T1 audit T2 compute T3 formal
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We study the non-factorizable corrections to W-pair-mediated four-fermion production in ee annihilation in double-pole approximation. We show how these corrections can be combined with the known corrections to the production and the decay of on-shell W-boson pairs, and how the full off-shell Coulomb singularity is included. Moreover, we find that the actual form of the real non-factorizable corrections depends on the parametrization of phase space, more precisely, on the definition of the invariant masses of the resonant W bosons. For the usual parametrization the full analytical results for the non-factorizable corrections are presented. Our analytical and numerical results for the non-factorizable corrections agree with a recent calculation, which was found to differ from a previous one. The detailed numerical discussion covers the invariant-mass distribution, various angular distributions, and the lepton-energy distribution for leptonic final states.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Towards NNLO QCD predictions for off-shell top-quark pair production and decays

    hep-ph 2025-07 conditional novelty 8.0 of 10

    The first NNLO QCD prediction for off-shell W+W-bbbar production with massive bottom quarks at the LHC, using a double-pole approximation for the two-loop virtual and an on-shell matching for non-factorisable corrections.

  2. Probing Yoctosecond Quantum Dynamics in Toponium Formation at Colliders

    hep-ph 2025-07 reject novelty 5.0 of 10

    The authors claim that R_b near 343 GeV can separate instantaneous from delayed toponium formation at more than 5 sigma, but the delayed scenario is parameterized by an undetermined constant A.

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