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Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb

Prompt charm production in $pp$ collisions at a centre-of-mass energy of 7 TeV is measured with the decay $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$, using an integrated luminosity of 15.0 nb$ ^{-1}$ collected by the LHCb detector at CERN. The measurement is carried out in two-dimensional bins of...

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Autor principal: Hampson, Thomas R
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:http://cds.cern.ch/record/1670276
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author Hampson, Thomas R
author_facet Hampson, Thomas R
author_sort Hampson, Thomas R
collection CERN
description Prompt charm production in $pp$ collisions at a centre-of-mass energy of 7 TeV is measured with the decay $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$, using an integrated luminosity of 15.0 nb$ ^{-1}$ collected by the LHCb detector at CERN. The measurement is carried out in two-dimensional bins of $D^{0}$ rapidity and transverse momentum in the region $2.0 < y < 4.5$ and $0 < p_{\mathrm{T}} < 8\,\mathrm{GeV}/c$. The results are found to have excellent agreement with those measured using the decay $D^{0}\rightarrow K^{-}\pi^{+}$. With 1.0 fb $^{-1}$ of integrated luminosity, the time dependent ratio of $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ to $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$ decays is used to determine the ratio of doubly Cabibbo suppressed to Cabibbo favoured decay rates \begin{eqnarray*} r_{D}^{2}=\left(0.341\pm0.017\pm0.006\right)\% \end{eqnarray*} where the first uncertainty is statistical and the second is systematic. This is a previously unmeasured quantity, and can be used to measure the branching fraction of the doubly Cabibbo suppressed decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ \begin{eqnarray*} \mathcal{B}\left(D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}\right) \mathrm{\, via \,\, DCS } = \left(2.75\pm0.14\pm0.05\pm0.07\right)\times10^{-4} \end{eqnarray*} where the final uncertainty is from the branching fraction of the Cabibbo favoured decay $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$. In addition, the no-mixing hypothesis is excluded with a probability that corresponds to 2.8 standard deviations, and the time-integrated mixing rate is measured as $R_{M}=\left( 0.04 \pm 0.88 \right)\times 10^{-4}$.
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spelling cern-16702762019-09-30T06:29:59Zhttp://cds.cern.ch/record/1670276engHampson, Thomas RMeasurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCbParticle Physics - ExperimentPrompt charm production in $pp$ collisions at a centre-of-mass energy of 7 TeV is measured with the decay $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$, using an integrated luminosity of 15.0 nb$ ^{-1}$ collected by the LHCb detector at CERN. The measurement is carried out in two-dimensional bins of $D^{0}$ rapidity and transverse momentum in the region $2.0 < y < 4.5$ and $0 < p_{\mathrm{T}} < 8\,\mathrm{GeV}/c$. The results are found to have excellent agreement with those measured using the decay $D^{0}\rightarrow K^{-}\pi^{+}$. With 1.0 fb $^{-1}$ of integrated luminosity, the time dependent ratio of $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ to $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$ decays is used to determine the ratio of doubly Cabibbo suppressed to Cabibbo favoured decay rates \begin{eqnarray*} r_{D}^{2}=\left(0.341\pm0.017\pm0.006\right)\% \end{eqnarray*} where the first uncertainty is statistical and the second is systematic. This is a previously unmeasured quantity, and can be used to measure the branching fraction of the doubly Cabibbo suppressed decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ \begin{eqnarray*} \mathcal{B}\left(D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}\right) \mathrm{\, via \,\, DCS } = \left(2.75\pm0.14\pm0.05\pm0.07\right)\times10^{-4} \end{eqnarray*} where the final uncertainty is from the branching fraction of the Cabibbo favoured decay $D^{0}\rightarrow K^{-}\pi^{+}\pi^{-}\pi^{+}$. In addition, the no-mixing hypothesis is excluded with a probability that corresponds to 2.8 standard deviations, and the time-integrated mixing rate is measured as $R_{M}=\left( 0.04 \pm 0.88 \right)\times 10^{-4}$.CERN-THESIS-2013-291oai:cds.cern.ch:16702762014-03-21T14:08:04Z
spellingShingle Particle Physics - Experiment
Hampson, Thomas R
Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title_full Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title_fullStr Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title_full_unstemmed Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title_short Measurement of prompt charm production and the decay $D^{0}\rightarrow K^{+}\pi^{-}\pi^{+}\pi^{-}$ at LHCb
title_sort measurement of prompt charm production and the decay $d^{0}\rightarrow k^{+}\pi^{-}\pi^{+}\pi^{-}$ at lhcb
topic Particle Physics - Experiment
url http://cds.cern.ch/record/1670276
work_keys_str_mv AT hampsonthomasr measurementofpromptcharmproductionandthedecayd0rightarrowkpipipiatlhcb