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Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV

In this analysis we present the first results of the measurement of the shape parameter r$_{b}$ in the Lund-Bowler fragmentation function for the b quark in a $t$$\bar{t}$ environment. The analysis uses charmed mesons produced in the leptonic decays of $t$$\bar{t}$ at $\sqrt{s}$ = 13 TeV in the CMS...

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Autor principal: Yates, Brent
Lenguaje:eng
Publicado: 2019
Materias:
Acceso en línea:http://cds.cern.ch/record/2711964
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author Yates, Brent
author_facet Yates, Brent
author_sort Yates, Brent
collection CERN
description In this analysis we present the first results of the measurement of the shape parameter r$_{b}$ in the Lund-Bowler fragmentation function for the b quark in a $t$$\bar{t}$ environment. The analysis uses charmed mesons produced in the leptonic decays of $t$$\bar{t}$ at $\sqrt{s}$ = 13 TeV in the CMS detector using the full 2016 dataset with an integrated luminosity of 35.9 fb$^{-1}$. The charged particle decays of J/$\psi$ $\rightarrow$ $\mu$$^{+}$$\mu$$^{-}$ and D$^{0}$ $\rightarrow$ K$\pm$$\mu$$\mp$ are used as proxies for the parent b quark via the ratio x$_{B}$(the $p$$_{T}$ of the charmed meson divided by the $\sum$E$p$$_{T}^{ch}$ of all charged particles in the jet containing the meson) to measure the shape parameter r$_{b}$. The shape parameter r$_{b}$ is measured to be r$_{b}$ = 0.841$\pm$0.014(stat)$\pm$0.010 (syst)$_{+0.033}^{-0.026}$(FSR).
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language eng
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spelling oai-inspirehep.net-17731612020-03-03T23:24:37Zhttp://cds.cern.ch/record/2711964engYates, BrentMeasurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeVParticle Physics - ExperimentIn this analysis we present the first results of the measurement of the shape parameter r$_{b}$ in the Lund-Bowler fragmentation function for the b quark in a $t$$\bar{t}$ environment. The analysis uses charmed mesons produced in the leptonic decays of $t$$\bar{t}$ at $\sqrt{s}$ = 13 TeV in the CMS detector using the full 2016 dataset with an integrated luminosity of 35.9 fb$^{-1}$. The charged particle decays of J/$\psi$ $\rightarrow$ $\mu$$^{+}$$\mu$$^{-}$ and D$^{0}$ $\rightarrow$ K$\pm$$\mu$$\mp$ are used as proxies for the parent b quark via the ratio x$_{B}$(the $p$$_{T}$ of the charmed meson divided by the $\sum$E$p$$_{T}^{ch}$ of all charged particles in the jet containing the meson) to measure the shape parameter r$_{b}$. The shape parameter r$_{b}$ is measured to be r$_{b}$ = 0.841$\pm$0.014(stat)$\pm$0.010 (syst)$_{+0.033}^{-0.026}$(FSR).CERN-THESIS-2019-314oai:inspirehep.net:17731612019
spellingShingle Particle Physics - Experiment
Yates, Brent
Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title_full Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title_fullStr Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title_full_unstemmed Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title_short Measurement of the Shape of the b Quark Fragmentation Function Using Charmed Mesons in Proton-Proton Collisions at a Center of Mass-Energy of 13 TeV
title_sort measurement of the shape of the b quark fragmentation function using charmed mesons in proton-proton collisions at a center of mass-energy of 13 tev
topic Particle Physics - Experiment
url http://cds.cern.ch/record/2711964
work_keys_str_mv AT yatesbrent measurementoftheshapeofthebquarkfragmentationfunctionusingcharmedmesonsinprotonprotoncollisionsatacenterofmassenergyof13tev