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Measurement of the top-antitop mass difference

The standard model of particle physics is a local gauge-invariant quantum field theory in which the CPT symmetry plays a fundamental role. One of the consequences of CPT invariance is an equal mass for a particle and its antiparticle. In order to test the CPT invariance, we performed a measurement o...

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Autor principal: Van Onsem, Gerrit Patrick
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:http://cds.cern.ch/record/1495756
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author Van Onsem, Gerrit Patrick
author_facet Van Onsem, Gerrit Patrick
author_sort Van Onsem, Gerrit Patrick
collection CERN
description The standard model of particle physics is a local gauge-invariant quantum field theory in which the CPT symmetry plays a fundamental role. One of the consequences of CPT invariance is an equal mass for a particle and its antiparticle. In order to test the CPT invariance, we performed a measurement of the mass difference between the top and the antitop quark ($\Delta m_{\text{t}} = m_{\mathrm{t}} - m_{\overline{\mathrm{t}}}$) using events with a muon or an electron and at least four jets in the final state. The analysis is based on data collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of $4.96 \pm 0.11$~fb$^{-1}$, and yields the value of $\Delta m_{\text{t}} = -0.44 \pm 0.46 ~(\text{stat.}) \pm 0.27 ~(\text{syst.})~\text{GeV}$. This result is consistent with equality of particle and antiparticle masses required by CPT invariance, and provides a significantly improved precision relative to existing measurements.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-14957562019-09-30T06:29:59Zhttp://cds.cern.ch/record/1495756engVan Onsem, Gerrit PatrickMeasurement of the top-antitop mass differenceDetectors and Experimental TechniquesThe standard model of particle physics is a local gauge-invariant quantum field theory in which the CPT symmetry plays a fundamental role. One of the consequences of CPT invariance is an equal mass for a particle and its antiparticle. In order to test the CPT invariance, we performed a measurement of the mass difference between the top and the antitop quark ($\Delta m_{\text{t}} = m_{\mathrm{t}} - m_{\overline{\mathrm{t}}}$) using events with a muon or an electron and at least four jets in the final state. The analysis is based on data collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of $4.96 \pm 0.11$~fb$^{-1}$, and yields the value of $\Delta m_{\text{t}} = -0.44 \pm 0.46 ~(\text{stat.}) \pm 0.27 ~(\text{syst.})~\text{GeV}$. This result is consistent with equality of particle and antiparticle masses required by CPT invariance, and provides a significantly improved precision relative to existing measurements.CMS-CR-2012-317oai:cds.cern.ch:14957562012-11-21
spellingShingle Detectors and Experimental Techniques
Van Onsem, Gerrit Patrick
Measurement of the top-antitop mass difference
title Measurement of the top-antitop mass difference
title_full Measurement of the top-antitop mass difference
title_fullStr Measurement of the top-antitop mass difference
title_full_unstemmed Measurement of the top-antitop mass difference
title_short Measurement of the top-antitop mass difference
title_sort measurement of the top-antitop mass difference
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1495756
work_keys_str_mv AT vanonsemgerritpatrick measurementofthetopantitopmassdifference