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Measurement of the Z to tau tau cross section with the ATLAS detector

The $Z$ to tau tau cross section has been measured using data at $\sqrt s = 7~\mathrm{TeV}$ collected with the ATLAS detector at the LHC corresponding to the integrated luminosity of $1.34 - 1.55~\mathrm{fb}^{-1}$. The analysis is performed in three different final states determined by decay modes o...

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Detalles Bibliográficos
Autor principal: Novakova, J
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:http://cds.cern.ch/record/1494130
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author Novakova, J
author_facet Novakova, J
author_sort Novakova, J
collection CERN
description The $Z$ to tau tau cross section has been measured using data at $\sqrt s = 7~\mathrm{TeV}$ collected with the ATLAS detector at the LHC corresponding to the integrated luminosity of $1.34 - 1.55~\mathrm{fb}^{-1}$. The analysis is performed in three different final states determined by decay modes of the tau leptons. Cross sections are measured separately in each final state in a fiducial kinematic phase space and extrapolated to the full phase space in the invariant mass region $66 - 116~\mathrm{GeV}$. The individual cross sections are combined together and the product of the total $Z$ boson production cross section and the $Z \rightarrow \tau\tau$ branching fraction is measured to be $0.92 \pm 0.20~\mathrm{(stat)}~\pm 0.08~\mathrm{(syst)}~\pm 0.03~\mathrm{(lumi)~nb}$, in agreement with the NNLO theoretical expectations.
id cern-1494130
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2012
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spelling cern-14941302019-09-30T06:29:59Zhttp://cds.cern.ch/record/1494130engNovakova, JMeasurement of the Z to tau tau cross section with the ATLAS detectorDetectors and Experimental TechniquesThe $Z$ to tau tau cross section has been measured using data at $\sqrt s = 7~\mathrm{TeV}$ collected with the ATLAS detector at the LHC corresponding to the integrated luminosity of $1.34 - 1.55~\mathrm{fb}^{-1}$. The analysis is performed in three different final states determined by decay modes of the tau leptons. Cross sections are measured separately in each final state in a fiducial kinematic phase space and extrapolated to the full phase space in the invariant mass region $66 - 116~\mathrm{GeV}$. The individual cross sections are combined together and the product of the total $Z$ boson production cross section and the $Z \rightarrow \tau\tau$ branching fraction is measured to be $0.92 \pm 0.20~\mathrm{(stat)}~\pm 0.08~\mathrm{(syst)}~\pm 0.03~\mathrm{(lumi)~nb}$, in agreement with the NNLO theoretical expectations.ATL-PHYS-PROC-2012-248oai:cds.cern.ch:14941302012-11-15
spellingShingle Detectors and Experimental Techniques
Novakova, J
Measurement of the Z to tau tau cross section with the ATLAS detector
title Measurement of the Z to tau tau cross section with the ATLAS detector
title_full Measurement of the Z to tau tau cross section with the ATLAS detector
title_fullStr Measurement of the Z to tau tau cross section with the ATLAS detector
title_full_unstemmed Measurement of the Z to tau tau cross section with the ATLAS detector
title_short Measurement of the Z to tau tau cross section with the ATLAS detector
title_sort measurement of the z to tau tau cross section with the atlas detector
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1494130
work_keys_str_mv AT novakovaj measurementoftheztotautaucrosssectionwiththeatlasdetector