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Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment

The production of the Higgs boson in association with the top quarks allows a direct measurement of the Yukawa coupling as a key parameter of the Standard Model. A search for such process in multilepton final states mainly targeting the decays $\rm H \to WW^*$, $\tau\tau$, and $ZZ^*$ is performed us...

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Detalles Bibliográficos
Autor principal: Ali, Babar
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.22323/1.282.1137
http://cds.cern.ch/record/2231818
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author Ali, Babar
author_facet Ali, Babar
author_sort Ali, Babar
collection CERN
description The production of the Higgs boson in association with the top quarks allows a direct measurement of the Yukawa coupling as a key parameter of the Standard Model. A search for such process in multilepton final states mainly targeting the decays $\rm H \to WW^*$, $\tau\tau$, and $ZZ^*$ is performed using 13.2 $\rm \mathrm{fb}^{-1}$ of data recorded by the ATLAS detector in 2015 and 2016 at a center of mass energy $\sqrt{s} = 13$~TeV. An overview of the final state with two same-charge light leptons ($\rm e$ or $\rm \mu$) and one hadronically-decaying $\rm \tau$ is described in more detail. The best-fit value of the ratio of observed and Standard Model cross sections for the combined multilepton final states is 2.5$\pm$0.7(stat)$^{+1.1}_{-0.9}$(syst), which is consistent with the Standard Model expectation.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-22318182019-09-30T06:29:59Zdoi:10.22323/1.282.1137http://cds.cern.ch/record/2231818engAli, BabarTop associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experimentParticle Physics - ExperimentThe production of the Higgs boson in association with the top quarks allows a direct measurement of the Yukawa coupling as a key parameter of the Standard Model. A search for such process in multilepton final states mainly targeting the decays $\rm H \to WW^*$, $\tau\tau$, and $ZZ^*$ is performed using 13.2 $\rm \mathrm{fb}^{-1}$ of data recorded by the ATLAS detector in 2015 and 2016 at a center of mass energy $\sqrt{s} = 13$~TeV. An overview of the final state with two same-charge light leptons ($\rm e$ or $\rm \mu$) and one hadronically-decaying $\rm \tau$ is described in more detail. The best-fit value of the ratio of observed and Standard Model cross sections for the combined multilepton final states is 2.5$\pm$0.7(stat)$^{+1.1}_{-0.9}$(syst), which is consistent with the Standard Model expectation.ATL-PHYS-PROC-2016-215oai:cds.cern.ch:22318182016-11-10
spellingShingle Particle Physics - Experiment
Ali, Babar
Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title_full Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title_fullStr Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title_full_unstemmed Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title_short Top associated Higgs boson production channel $ \rm \mathbf{ttH\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ TeV with the ATLAS experiment
title_sort top associated higgs boson production channel $ \rm \mathbf{tth\rightarrow 2\ell + 1 \tau_{had}}$ at $\mathbf{\sqrt{s}= 13}$ tev with the atlas experiment
topic Particle Physics - Experiment
url https://dx.doi.org/10.22323/1.282.1137
http://cds.cern.ch/record/2231818
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