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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.95.034042 http://cds.cern.ch/record/2221411 |
_version_ | 1780952235705892864 |
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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 |
work_keys_str_mv | AT aliolisimone zzproductioningluonfusionatnlomatchedtopartonshower AT caolafabrizio zzproductioningluonfusionatnlomatchedtopartonshower AT luisonigionata zzproductioningluonfusionatnlomatchedtopartonshower AT rontschraul zzproductioningluonfusionatnlomatchedtopartonshower |