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QCD corrections to $W^+W^-$ production through gluon fusion

We compute the next-to-leading order (NLO) QCD corrections to the $gg \to W^+ W^- \to l^+_1 \nu_1 l^-_2 \bar \nu_2$ process, mediated by a massless quark loop, at the LHC. This process first contributes to the hadroproduction of $W^+W^-$ at $\mathcal{O}(\alpha_s^2)$, but, nevertheless, has a sizable...

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Autores principales: Caola, Fabrizio, Melnikov, Kirill, Röntsch, Raoul, Tancredi, Lorenzo
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2016.01.046
http://cds.cern.ch/record/2109129
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author Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
Tancredi, Lorenzo
author_facet Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
Tancredi, Lorenzo
author_sort Caola, Fabrizio
collection CERN
description We compute the next-to-leading order (NLO) QCD corrections to the $gg \to W^+ W^- \to l^+_1 \nu_1 l^-_2 \bar \nu_2$ process, mediated by a massless quark loop, at the LHC. This process first contributes to the hadroproduction of $W^+W^-$ at $\mathcal{O}(\alpha_s^2)$, but, nevertheless, has a sizable impact on the total production rate. We find that the NLO QCD corrections to the $gg \to W^+W^-$ process amount to ${\cal O}(50)$%, and increase the NNLO QCD cross sections of $pp \to W^+W^-$ by approximately two percent, at both the 8 TeV and 13 TeV LHC. We also compute the NLO corrections to gluonic $W^+W^-$ production within a fiducial volume used by the ATLAS collaboration in their 8 TeV measurement of the $W^+W^-$ production rate and find that the QCD corrections are significantly smaller than in the inclusive case. While the current experimental uncertainties are still too large to make these differences relevant, the observed strong dependence of perturbative corrections on kinematic cuts underscores that extrapolation from a fiducial measurement to the total cross section is an extremely delicate matter, and calls for the direct comparison of fiducial volume measurements with corresponding theoretical computations.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2015
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spelling cern-21091292022-08-10T12:45:10Zdoi:10.1016/j.physletb.2016.01.046http://cds.cern.ch/record/2109129engCaola, FabrizioMelnikov, KirillRöntsch, RaoulTancredi, LorenzoQCD corrections to $W^+W^-$ production through gluon fusionParticle Physics - PhenomenologyWe compute the next-to-leading order (NLO) QCD corrections to the $gg \to W^+ W^- \to l^+_1 \nu_1 l^-_2 \bar \nu_2$ process, mediated by a massless quark loop, at the LHC. This process first contributes to the hadroproduction of $W^+W^-$ at $\mathcal{O}(\alpha_s^2)$, but, nevertheless, has a sizable impact on the total production rate. We find that the NLO QCD corrections to the $gg \to W^+W^-$ process amount to ${\cal O}(50)$%, and increase the NNLO QCD cross sections of $pp \to W^+W^-$ by approximately two percent, at both the 8 TeV and 13 TeV LHC. We also compute the NLO corrections to gluonic $W^+W^-$ production within a fiducial volume used by the ATLAS collaboration in their 8 TeV measurement of the $W^+W^-$ production rate and find that the QCD corrections are significantly smaller than in the inclusive case. While the current experimental uncertainties are still too large to make these differences relevant, the observed strong dependence of perturbative corrections on kinematic cuts underscores that extrapolation from a fiducial measurement to the total cross section is an extremely delicate matter, and calls for the direct comparison of fiducial volume measurements with corresponding theoretical computations.We compute the next-to-leading order (NLO) QCD corrections to the $gg \to W^+ W^- \to l^+_1 \nu_1 l^-_2 \bar \nu_2$ process, mediated by a massless quark loop, at the LHC. This process first contributes to the hadroproduction of $W^+W^-$ at $\mathcal{O}(\alpha_s^2)$, but, nevertheless, has a sizable impact on the total production rate. We find that the NLO QCD corrections to the $gg \to W^+W^-$ process amount to ${\cal O}(50)$%, and increase the NNLO QCD cross sections of $pp \to W^+W^-$ by approximately two percent, at both the 8 TeV and 13 TeV LHC. We also compute the NLO corrections to gluonic $W^+W^-$ production within a fiducial volume used by the ATLAS collaboration in their 8 TeV measurement of the $W^+W^-$ production rate and find that the QCD corrections are significantly smaller than in the inclusive case. While the current experimental uncertainties are still too large to make these differences relevant, the observed strong dependence of perturbative corrections on kinematic cuts underscores that extrapolation from a fiducial measurement to the total cross section is an extremely delicate matter, and calls for the direct comparison of fiducial volume measurements with corresponding theoretical computations.We compute the next-to-leading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 process, mediated by a massless quark loop, at the LHC. This process first contributes to the hadroproduction of W+W− at O(αs2) , but, nevertheless, has a sizable impact on the total production rate. We find that the NLO QCD corrections to the gg→W+W− process amount to O(50)% , and increase the NNLO QCD cross sections of pp→W+W− by approximately two percent, at both the 8 TeV and 13 TeV LHC. We also compute the NLO corrections to gluonic W+W− production within a fiducial volume used by the ATLAS Collaboration in their 8 TeV measurement of the W+W− production rate and find that the QCD corrections are significantly smaller than in the inclusive case. While the current experimental uncertainties are still too large to make these differences relevant, the observed strong dependence of perturbative corrections on kinematic cuts underscores that extrapolation from a fiducial measurement to the total cross section is an extremely delicate matter, and calls for the direct comparison of fiducial volume measurements with corresponding theoretical computations.CERN-PH-TH-2015-276TTP15-041arXiv:1511.08617CERN-PH-TH-2015-276TTP15-041oai:cds.cern.ch:21091292015-11-27
spellingShingle Particle Physics - Phenomenology
Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
Tancredi, Lorenzo
QCD corrections to $W^+W^-$ production through gluon fusion
title QCD corrections to $W^+W^-$ production through gluon fusion
title_full QCD corrections to $W^+W^-$ production through gluon fusion
title_fullStr QCD corrections to $W^+W^-$ production through gluon fusion
title_full_unstemmed QCD corrections to $W^+W^-$ production through gluon fusion
title_short QCD corrections to $W^+W^-$ production through gluon fusion
title_sort qcd corrections to $w^+w^-$ production through gluon fusion
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2016.01.046
http://cds.cern.ch/record/2109129
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AT melnikovkirill qcdcorrectionstowwproductionthroughgluonfusion
AT rontschraoul qcdcorrectionstowwproductionthroughgluonfusion
AT tancredilorenzo qcdcorrectionstowwproductionthroughgluonfusion