W+ W− boson pair production in proton-proton collisions at √s=13  TeV

Bibliographic Details
Main Author: Sirunyan, A. M.
Publication Date: 2020
Other Authors: Silveira, Gustavo Gil da, CMS Collaboration
Format: Article
Language: eng
Source: Repositório Institucional da UFRGS
Download full: http://hdl.handle.net/10183/216891
Summary: A measurement of the W+W− boson pair production cross section in proton-proton collisions at s=13  TeV is presented. The data used in this study are collected with the CMS detector at the CERN LHC and correspond to an integrated luminosity of 35.9  fb−1. The W+W− candidate events are selected by requiring two oppositely charged leptons (electrons or muons). Two methods for reducing background contributions are employed. In the first one, a sequence of requirements on kinematic quantities is applied allowing a measurement of the total production cross section, 117.6±6.8  pb, which agrees well with the theoretical prediction. Fiducial cross sections are also reported for events with zero or one jet, and the change in the zero-jet fiducial cross section with the jet transverse momentum threshold is measured. Normalized differential cross sections are reported within the fiducial region. A second method for suppressing background contributions employs two random forest classifiers. The analysis based on this method includes a measurement of the total production cross section and also a measurement of the normalized jet multiplicity distribution in W+W− events. Finally, a dilepton invariant mass distribution is used to probe for physics beyond the standard model in the context of an effective field theory, and constraints on the presence of dimension-6 operators are derived.
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spelling Sirunyan, A. M.Silveira, Gustavo Gil daCMS Collaboration2020-12-24T04:21:39Z20200556-2821http://hdl.handle.net/10183/216891001120319A measurement of the W+W− boson pair production cross section in proton-proton collisions at s=13  TeV is presented. The data used in this study are collected with the CMS detector at the CERN LHC and correspond to an integrated luminosity of 35.9  fb−1. The W+W− candidate events are selected by requiring two oppositely charged leptons (electrons or muons). Two methods for reducing background contributions are employed. In the first one, a sequence of requirements on kinematic quantities is applied allowing a measurement of the total production cross section, 117.6±6.8  pb, which agrees well with the theoretical prediction. Fiducial cross sections are also reported for events with zero or one jet, and the change in the zero-jet fiducial cross section with the jet transverse momentum threshold is measured. Normalized differential cross sections are reported within the fiducial region. A second method for suppressing background contributions employs two random forest classifiers. The analysis based on this method includes a measurement of the total production cross section and also a measurement of the normalized jet multiplicity distribution in W+W− events. Finally, a dilepton invariant mass distribution is used to probe for physics beyond the standard model in the context of an effective field theory, and constraints on the presence of dimension-6 operators are derived.application/pdfengPhysical Review. D, Particles and fields. Woodbury. Vol. 102, no. 9 (Nov. 2020), 092001, 30 p.Aceleradores de partículasColisões proton-protonBosons WW+ W− boson pair production in proton-proton collisions at √s=13  TeVEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT001120319.pdf.txt001120319.pdf.txtExtracted Texttext/plain147012http://www.lume.ufrgs.br/bitstream/10183/216891/2/001120319.pdf.txta8db57e4f3d72a205030f9f37c9d2f1cMD52ORIGINAL001120319.pdfTexto completo (inglês)application/pdf1626909http://www.lume.ufrgs.br/bitstream/10183/216891/1/001120319.pdf238421da2e41c5a3ebf67b4b5c420c7eMD5110183/2168912023-07-22 03:41:36.125965oai:www.lume.ufrgs.br:10183/216891Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-07-22T06:41:36Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv W+ W− boson pair production in proton-proton collisions at √s=13  TeV
title W+ W− boson pair production in proton-proton collisions at √s=13  TeV
spellingShingle W+ W− boson pair production in proton-proton collisions at √s=13  TeV
Sirunyan, A. M.
Aceleradores de partículas
Colisões proton-proton
Bosons W
title_short W+ W− boson pair production in proton-proton collisions at √s=13  TeV
title_full W+ W− boson pair production in proton-proton collisions at √s=13  TeV
title_fullStr W+ W− boson pair production in proton-proton collisions at √s=13  TeV
title_full_unstemmed W+ W− boson pair production in proton-proton collisions at √s=13  TeV
title_sort W+ W− boson pair production in proton-proton collisions at √s=13  TeV
author Sirunyan, A. M.
author_facet Sirunyan, A. M.
Silveira, Gustavo Gil da
CMS Collaboration
author_role author
author2 Silveira, Gustavo Gil da
CMS Collaboration
author2_role author
author
dc.contributor.author.fl_str_mv Sirunyan, A. M.
Silveira, Gustavo Gil da
CMS Collaboration
dc.subject.por.fl_str_mv Aceleradores de partículas
Colisões proton-proton
Bosons W
topic Aceleradores de partículas
Colisões proton-proton
Bosons W
description A measurement of the W+W− boson pair production cross section in proton-proton collisions at s=13  TeV is presented. The data used in this study are collected with the CMS detector at the CERN LHC and correspond to an integrated luminosity of 35.9  fb−1. The W+W− candidate events are selected by requiring two oppositely charged leptons (electrons or muons). Two methods for reducing background contributions are employed. In the first one, a sequence of requirements on kinematic quantities is applied allowing a measurement of the total production cross section, 117.6±6.8  pb, which agrees well with the theoretical prediction. Fiducial cross sections are also reported for events with zero or one jet, and the change in the zero-jet fiducial cross section with the jet transverse momentum threshold is measured. Normalized differential cross sections are reported within the fiducial region. A second method for suppressing background contributions employs two random forest classifiers. The analysis based on this method includes a measurement of the total production cross section and also a measurement of the normalized jet multiplicity distribution in W+W− events. Finally, a dilepton invariant mass distribution is used to probe for physics beyond the standard model in the context of an effective field theory, and constraints on the presence of dimension-6 operators are derived.
publishDate 2020
dc.date.accessioned.fl_str_mv 2020-12-24T04:21:39Z
dc.date.issued.fl_str_mv 2020
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dc.identifier.issn.pt_BR.fl_str_mv 0556-2821
dc.identifier.nrb.pt_BR.fl_str_mv 001120319
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url http://hdl.handle.net/10183/216891
dc.language.iso.fl_str_mv eng
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dc.relation.ispartof.pt_BR.fl_str_mv Physical Review. D, Particles and fields. Woodbury. Vol. 102, no. 9 (Nov. 2020), 092001, 30 p.
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