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Electroweak W+W-jj prodution at NLO in QCD matched with parton shower in the POWHEG-BOX

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arxiv 1301.1695 v1 pith:TIHKDLKX submitted 2013-01-08 hep-ph hep-ex

classification hep-phhep-ex
keywords partonshowerbosonselectroweakimpactimplementationnext-to-leadingorder
verification ladder T0 review T1 audit T2 compute T3 formal
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We present an implementation of electroweak W+W-jj production at hadron colliders in the POWHEG framework, a method that allows the interfacing of a next-to-leading order QCD calculation with parton shower Monte Carlo programs. We provide results for both, fully and semi-leptonic decay modes of the weak bosons, taking resonant and non-resonant contributions and spin correlations of the final-state particles into account. To illustrate the versatility of our implementation, we provide phenomenological results for two representative scenarios with a light and with a heavy Higgs boson, respectively, and in a kinematic regime of highly boosted gauge bosons. The impact of the parton shower is found to depend on the setup and the observable under investigation. In particular, distributions related to a central-jet veto are more sensitive to these effects. Therefore the impact of radiation by the parton shower on next-to-leading order predictions should be assessed carefully on a case-by-case basis.

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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. Precision tools for the simulation of double-Higgs production via vector-boson fusion

    hep-ph 2025-02 accept novelty 6.0 of 10

    New and extended Monte Carlo tools for vector-boson-fusion double-Higgs production now support anomalous Higgs couplings, and show that NLO-plus-shower predictions approximate NNLO results while non-factorizable QCD c...

  2. NLO QCD and EW corrections to semileptonic vector-boson scattering at the LHC

    hep-ph 2026-06 unverdicted novelty 4.0 of 10

    NLO QCD and EW corrections computed for semileptonic vector-boson scattering in two fiducial regions at the LHC.

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