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Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer

Leptonic decays of W/Z bosons provide the first electroweak precision measurements at the Large Hadron Collider (LHC). The results of measurements of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}=7 \mathrm{TeV}$ are presented, based on 2.9 pb$^{-1}$ of data recorded...

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Autor principal: Werner, Jeremy
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:http://cds.cern.ch/record/1362325
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author Werner, Jeremy
author_facet Werner, Jeremy
author_sort Werner, Jeremy
collection CERN
description Leptonic decays of W/Z bosons provide the first electroweak precision measurements at the Large Hadron Collider (LHC). The results of measurements of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}=7 \mathrm{TeV}$ are presented, based on 2.9 pb$^{-1}$ of data recorded by the Compact Muon Solenoid (CMS) detector at the LHC. The measurements, performed in the electron and muon decay channels, are combined to give $\sigma(\mathrm{pp} \rightarrow \mathrm{W}X) \times {\cal{B}}(\mathrm{W} \rightarrow \ell \nu)$ = $9.95\pm0.07\,{\textrm{(stat.)}}\pm 0.28\,{\textrm{(syst.)}}\pm1.09\,{\textrm{(lumi.)}} \mathrm{nb}$ and $\sigma(\mathrm{pp} \rightarrow \mathrm{Z}X) \times {\cal{B}}(\mathrm{Z} \rightarrow \ell^+ \ell^-)$ = $0.931\pm0.026\,{\textrm{(stat.)}}\pm 0.023\,{\textrm{(syst.)}}\pm0.102\,{\textrm{(lumi.)}} \mathrm{nb}$, where $\ell$ stands for either $\mathrm{e}$ or $\mu$. Theoretical predictions, calculated at the next-to-next-to-leading order (NNLO) in QCD using recent parton distribution functions (PDFs), are in agreement with the measured cross sections. Hence copious production of these well understood and clean signatures suggest the use of W/Z as a "standard candle" for measuring the luminosity at the LHC alongside the current Van der Meer (VdM) separation scan method.
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spelling cern-13623252019-09-30T06:29:59Zhttp://cds.cern.ch/record/1362325engWerner, JeremyMeasurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a LuminometerParticle Physics - ExperimentLeptonic decays of W/Z bosons provide the first electroweak precision measurements at the Large Hadron Collider (LHC). The results of measurements of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}=7 \mathrm{TeV}$ are presented, based on 2.9 pb$^{-1}$ of data recorded by the Compact Muon Solenoid (CMS) detector at the LHC. The measurements, performed in the electron and muon decay channels, are combined to give $\sigma(\mathrm{pp} \rightarrow \mathrm{W}X) \times {\cal{B}}(\mathrm{W} \rightarrow \ell \nu)$ = $9.95\pm0.07\,{\textrm{(stat.)}}\pm 0.28\,{\textrm{(syst.)}}\pm1.09\,{\textrm{(lumi.)}} \mathrm{nb}$ and $\sigma(\mathrm{pp} \rightarrow \mathrm{Z}X) \times {\cal{B}}(\mathrm{Z} \rightarrow \ell^+ \ell^-)$ = $0.931\pm0.026\,{\textrm{(stat.)}}\pm 0.023\,{\textrm{(syst.)}}\pm0.102\,{\textrm{(lumi.)}} \mathrm{nb}$, where $\ell$ stands for either $\mathrm{e}$ or $\mu$. Theoretical predictions, calculated at the next-to-next-to-leading order (NNLO) in QCD using recent parton distribution functions (PDFs), are in agreement with the measured cross sections. Hence copious production of these well understood and clean signatures suggest the use of W/Z as a "standard candle" for measuring the luminosity at the LHC alongside the current Van der Meer (VdM) separation scan method.Leptonic decays of W/Z bosons provide the first electroweak precision measurements at the Large Hadron Collider (LHC). The results of measurements of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}=7 \mathrm{TeV}$ are presented, based on 2.9 pb$^{-1}$ of data recorded by the Compact Muon Solenoid (CMS) detector at the LHC. The measurements, performed in the electron and muon decay channels, are combined to give $\sigma(\mathrm{pp} \rightarrow \mathrm{W}X) \times {\cal{B}}(\mathrm{W} \rightarrow \ell \nu) = 9.95\pm0.07\,{\textrm{(stat.)}}\pm 0.28\,{\textrm{(syst.)}}\pm1.09\,{\textrm{(lumi.)}} \mathrm{nb}$ and $\sigma(\mathrm{pp} \rightarrow \mathrm{Z}X) \times {\cal{B}}(\mathrm{Z} \rightarrow \ell^+ \ell^-) = 0.931\pm0.026\,{\textrm{(stat.)}}\pm 0.023\,{\textrm{(syst.)}}\pm0.102\,{\textrm{(lumi.)}} \mathrm{nb}$, where $\ell$ stands for either $\mathrm{e}$ or $\mu$. Theoretical predictions, calculated at the next-to-next-to-leading order (NNLO) in QCD using recent parton distribution functions (PDFs), are in agreement with the measured cross sections. Hence copious production of these well understood and clean signatures suggest the use of W/Z as a "standard candle" for measuring the luminosity at the LHC alongside the current Van der Meer (VdM) separation scan method.arXiv:1106.5393CERN-PROCEEDINGS-2011-001-26-29oai:cds.cern.ch:13623252011-06-28
spellingShingle Particle Physics - Experiment
Werner, Jeremy
Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title_full Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title_fullStr Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title_full_unstemmed Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title_short Measurements of Inclusive W/Z Production Cross Sections at CMS and W/Z as a Luminometer
title_sort measurements of inclusive w/z production cross sections at cms and w/z as a luminometer
topic Particle Physics - Experiment
url http://cds.cern.ch/record/1362325
work_keys_str_mv AT wernerjeremy measurementsofinclusivewzproductioncrosssectionsatcmsandwzasaluminometer