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Overview of $C\!P$V parameter $\phi_{s}$ determination
The one of main goals of the LHCb experiment is the measurement of the mixing-induced $C\!P$-violating phase $\phi_{s}$ in the $B^{0}_{s}-\bar{B}^{0}_{s}$ system. It has been measured exploiting the Run~I data set, using several decay channels. The most recent results obtained analyzing $B^{0}_{s}\t...
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Lenguaje: | eng |
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2018
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Acceso en línea: | https://dx.doi.org/10.18502/ken.v3i1.1773 http://cds.cern.ch/record/2302050 |
_version_ | 1780957236394196992 |
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author | Batozskaya, Varvara |
author_facet | Batozskaya, Varvara |
author_sort | Batozskaya, Varvara |
collection | CERN |
description | The one of main goals of the LHCb experiment is the measurement of the mixing-induced $C\!P$-violating phase $\phi_{s}$ in the $B^{0}_{s}-\bar{B}^{0}_{s}$ system. It has been measured exploiting the Run~I data set, using several decay channels. The most recent results obtained analyzing $B^{0}_{s}\to J/\psi K^{+}K^{-}$ candidates in the $K^{+}K^{-}$ mass region above the $\phi(1020)$ resonance are presented. The measurements using the same final state with the $m(K^{+}K^{-})$ at the $\phi(1020)$ and $B^{0}_{s}\to J/\psi \pi^{+}\pi^{-}$, as well as using the $B^{0}_{s}\to \psi(2S)\phi$ decay are discussed. |
id | cern-2302050 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | cern-23020502021-05-03T08:04:24Zdoi:10.18502/ken.v3i1.1773http://cds.cern.ch/record/2302050engBatozskaya, VarvaraOverview of $C\!P$V parameter $\phi_{s}$ determinationParticle Physics - ExperimentThe one of main goals of the LHCb experiment is the measurement of the mixing-induced $C\!P$-violating phase $\phi_{s}$ in the $B^{0}_{s}-\bar{B}^{0}_{s}$ system. It has been measured exploiting the Run~I data set, using several decay channels. The most recent results obtained analyzing $B^{0}_{s}\to J/\psi K^{+}K^{-}$ candidates in the $K^{+}K^{-}$ mass region above the $\phi(1020)$ resonance are presented. The measurements using the same final state with the $m(K^{+}K^{-})$ at the $\phi(1020)$ and $B^{0}_{s}\to J/\psi \pi^{+}\pi^{-}$, as well as using the $B^{0}_{s}\to \psi(2S)\phi$ decay are discussed.LHCb-PROC-2018-008CERN-LHCb-PROC-2018-008oai:cds.cern.ch:23020502018-01-26 |
spellingShingle | Particle Physics - Experiment Batozskaya, Varvara Overview of $C\!P$V parameter $\phi_{s}$ determination |
title | Overview of $C\!P$V parameter $\phi_{s}$ determination |
title_full | Overview of $C\!P$V parameter $\phi_{s}$ determination |
title_fullStr | Overview of $C\!P$V parameter $\phi_{s}$ determination |
title_full_unstemmed | Overview of $C\!P$V parameter $\phi_{s}$ determination |
title_short | Overview of $C\!P$V parameter $\phi_{s}$ determination |
title_sort | overview of $c\!p$v parameter $\phi_{s}$ determination |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.18502/ken.v3i1.1773 http://cds.cern.ch/record/2302050 |
work_keys_str_mv | AT batozskayavarvara overviewofcpvparameterphisdetermination |