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ZZ production in gluon fusion at NLO matched to parton-shower

We present a calculation of the next-to-leading order (NLO) QCD corrections to the hadroproduction process $gg\to ZZ \to e^+e^- \mu^+ \mu^-$, matched to the parton shower in the POWHEG framework. We take advantage of the POWHEG BOX tool for the implementation and rely on PYTHIA 8 for the showering a...

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Detalles Bibliográficos
Autores principales: Alioli, Simone, Caola, Fabrizio, Luisoni, Gionata, Röntsch, Raul
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.95.034042
http://cds.cern.ch/record/2221411
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author Alioli, Simone
Caola, Fabrizio
Luisoni, Gionata
Röntsch, Raul
author_facet Alioli, Simone
Caola, Fabrizio
Luisoni, Gionata
Röntsch, Raul
author_sort Alioli, Simone
collection CERN
description We present a calculation of the next-to-leading order (NLO) QCD corrections to the hadroproduction process $gg\to ZZ \to e^+e^- \mu^+ \mu^-$, matched to the parton shower in the POWHEG framework. We take advantage of the POWHEG BOX tool for the implementation and rely on PYTHIA 8 for the showering and hadronization stages. We fully include $\gamma^*/Z$ interference effects, while also covering the single-resonant region. For this phenomenological study we focus on four lepton production as a signal process, neglecting all quark mass effects as well as the Higgs-mediated contributions, which are known to be subdominant in this case. We provide predictions from our simulations for the 13 TeV LHC Run II setup, including realistic experimental cuts.
id cern-2221411
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-22214112022-08-10T12:34:25Zdoi:10.1103/PhysRevD.95.034042http://cds.cern.ch/record/2221411engAlioli, SimoneCaola, FabrizioLuisoni, GionataRöntsch, RaulZZ production in gluon fusion at NLO matched to parton-showerhep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyWe present a calculation of the next-to-leading order (NLO) QCD corrections to the hadroproduction process $gg\to ZZ \to e^+e^- \mu^+ \mu^-$, matched to the parton shower in the POWHEG framework. We take advantage of the POWHEG BOX tool for the implementation and rely on PYTHIA 8 for the showering and hadronization stages. We fully include $\gamma^*/Z$ interference effects, while also covering the single-resonant region. For this phenomenological study we focus on four lepton production as a signal process, neglecting all quark mass effects as well as the Higgs-mediated contributions, which are known to be subdominant in this case. We provide predictions from our simulations for the 13 TeV LHC Run II setup, including realistic experimental cuts.We present a calculation of the next-to-leading order QCD corrections to the hadroproduction process gg→ZZ→e+e-μ+μ-, matched to the parton shower in the powheg framework. We take advantage of the powheg box tool for the implementation and rely on pythia8 for the showering and hadronization stages. We fully include γ*/Z interference effects, while also covering the single-resonant region. For this phenomenological study we focus on four lepton production as a signal process, neglecting all quark mass effects as well as the Higgs-mediated contributions, which are known to be subdominant in this case. We provide predictions from our simulations for the 13 TeV LHC Run II setup, including realistic experimental cuts.We present a calculation of the next-to-leading order (NLO) QCD corrections to the hadroproduction process $gg\to ZZ \to e^+e^- \mu^+ \mu^-$, matched to the parton shower in the POWHEG framework. We take advantage of the POWHEG BOX tool for the implementation and rely on PYTHIA 8 for the showering and hadronization stages. We fully include $\gamma^*/Z$ interference effects, while also covering the single-resonant region. For this phenomenological study we focus on four lepton production as a signal process, neglecting all quark mass effects as well as the Higgs-mediated contributions, which are known to be subdominant in this case. We provide predictions from our simulations for the 13 TeV LHC Run II setup, including realistic experimental cuts.CERN-TH-2016-197arXiv:1609.09719oai:cds.cern.ch:22214112016-09-30
spellingShingle hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
Alioli, Simone
Caola, Fabrizio
Luisoni, Gionata
Röntsch, Raul
ZZ production in gluon fusion at NLO matched to parton-shower
title ZZ production in gluon fusion at NLO matched to parton-shower
title_full ZZ production in gluon fusion at NLO matched to parton-shower
title_fullStr ZZ production in gluon fusion at NLO matched to parton-shower
title_full_unstemmed ZZ production in gluon fusion at NLO matched to parton-shower
title_short ZZ production in gluon fusion at NLO matched to parton-shower
title_sort zz production in gluon fusion at nlo matched to parton-shower
topic hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.95.034042
http://cds.cern.ch/record/2221411
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AT caolafabrizio zzproductioningluonfusionatnlomatchedtopartonshower
AT luisonigionata zzproductioningluonfusionatnlomatchedtopartonshower
AT rontschraul zzproductioningluonfusionatnlomatchedtopartonshower