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Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$

Using a dataset corresponding to an integrated luminosity of 3.0 fb$^{-1}$ collected in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV, the $B_s^0 \to \phi \phi$ branching fraction is measured to be \[ \mathcal{B}(B_s^0 \to \phi \phi) = ( 1.84 \pm 0.05 (\text{stat}) \pm 0.07 (\text{syst})...

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Detalles Bibliográficos
Autor principal: Morris, Adam
Lenguaje:eng
Publicado: 2015
Acceso en línea:http://cds.cern.ch/record/2062007
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author Morris, Adam
author_facet Morris, Adam
author_sort Morris, Adam
collection CERN
description Using a dataset corresponding to an integrated luminosity of 3.0 fb$^{-1}$ collected in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV, the $B_s^0 \to \phi \phi$ branching fraction is measured to be \[ \mathcal{B}(B_s^0 \to \phi \phi) = ( 1.84 \pm 0.05 (\text{stat}) \pm 0.07 (\text{syst}) \pm 0.11 (f_s/f_d) \pm 0.12 (\text{norm}) ) \times 10^{-5}, \] where $f_s/f_d$ represents the ratio of the $B_s^0$ to $B^0$ production cross-sections, and the $B^0 \to \phi K^*(892)^0$ decay mode is used for normalization. This is the most precise measurement of this branching fraction to date, representing a factor five reduction in the statistical uncertainty compared with the previous best measurement. A search for the decay $B^0 \to \phi \phi$ is also made. No signal is observed, and an upper limit on the branching fraction is set as \[ \mathcal{B}(B^0 \to \phi \phi) < 2.8 \times 10^{-8} \] at 90% confidence level. This is a factor of seven improvement compared to the previous best limit.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-20620072019-09-30T06:29:59Zhttp://cds.cern.ch/record/2062007engMorris, AdamMeasurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$Using a dataset corresponding to an integrated luminosity of 3.0 fb$^{-1}$ collected in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV, the $B_s^0 \to \phi \phi$ branching fraction is measured to be \[ \mathcal{B}(B_s^0 \to \phi \phi) = ( 1.84 \pm 0.05 (\text{stat}) \pm 0.07 (\text{syst}) \pm 0.11 (f_s/f_d) \pm 0.12 (\text{norm}) ) \times 10^{-5}, \] where $f_s/f_d$ represents the ratio of the $B_s^0$ to $B^0$ production cross-sections, and the $B^0 \to \phi K^*(892)^0$ decay mode is used for normalization. This is the most precise measurement of this branching fraction to date, representing a factor five reduction in the statistical uncertainty compared with the previous best measurement. A search for the decay $B^0 \to \phi \phi$ is also made. No signal is observed, and an upper limit on the branching fraction is set as \[ \mathcal{B}(B^0 \to \phi \phi) < 2.8 \times 10^{-8} \] at 90% confidence level. This is a factor of seven improvement compared to the previous best limit.Poster-2015-513oai:cds.cern.ch:20620072015-08-31
spellingShingle Morris, Adam
Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title_full Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title_fullStr Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title_full_unstemmed Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title_short Measurement of the $B^0_s\to\phi\phi$ branching fraction and search for the decay $B^0\to\phi\phi$
title_sort measurement of the $b^0_s\to\phi\phi$ branching fraction and search for the decay $b^0\to\phi\phi$
url http://cds.cern.ch/record/2062007
work_keys_str_mv AT morrisadam measurementoftheb0stophiphibranchingfractionandsearchforthedecayb0tophiphi