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Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC

This talk presents the analyses results of the diboson (WW or WZ) resonances production search in pp collisions at √s = 8 and 13 TeV with the ATLAS detector at the LHC with the semileptonic final state. As benchmark signal models Randall-Sundrum bulk model for KK G* → WW and Heavy Vector Triplet mod...

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Autor principal: Cheremushkina, E
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1134/S1063779617050100
http://cds.cern.ch/record/2304070
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author Cheremushkina, E
author_facet Cheremushkina, E
author_sort Cheremushkina, E
collection CERN
description This talk presents the analyses results of the diboson (WW or WZ) resonances production search in pp collisions at √s = 8 and 13 TeV with the ATLAS detector at the LHC with the semileptonic final state. As benchmark signal models Randall-Sundrum bulk model for KK G* → WW and Heavy Vector Triplet model for W′ → WZ and Z′ → WW are used. No significant excess for diboson resonances production is observed and upper limits on the production cross section times branching fraction of G*, W′ and Z′ are determined at 95% CL.
id oai-inspirehep.net-1622189
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2017
record_format invenio
spelling oai-inspirehep.net-16221892019-09-30T06:29:59Zdoi:10.1134/S1063779617050100http://cds.cern.ch/record/2304070engCheremushkina, ESemileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHCParticle Physics - ExperimentThis talk presents the analyses results of the diboson (WW or WZ) resonances production search in pp collisions at √s = 8 and 13 TeV with the ATLAS detector at the LHC with the semileptonic final state. As benchmark signal models Randall-Sundrum bulk model for KK G* → WW and Heavy Vector Triplet model for W′ → WZ and Z′ → WW are used. No significant excess for diboson resonances production is observed and upper limits on the production cross section times branching fraction of G*, W′ and Z′ are determined at 95% CL.oai:inspirehep.net:16221892017
spellingShingle Particle Physics - Experiment
Cheremushkina, E
Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title_full Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title_fullStr Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title_full_unstemmed Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title_short Semileptonic (lepton, neutrino and jets) $WW/WZ$ resonances searches at $\sqrt{s}$ = 8 and 13 TeV with the ATLAS detector at the LHC
title_sort semileptonic (lepton, neutrino and jets) $ww/wz$ resonances searches at $\sqrt{s}$ = 8 and 13 tev with the atlas detector at the lhc
topic Particle Physics - Experiment
url https://dx.doi.org/10.1134/S1063779617050100
http://cds.cern.ch/record/2304070
work_keys_str_mv AT cheremushkinae semileptonicleptonneutrinoandjetswwwzresonancessearchesatsqrts8and13tevwiththeatlasdetectoratthelhc