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2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb

A measurement of the phase of the $\rm B_s$-$\bar{\rm B}_s$ oscillation amplitude with respect to that of the ${\rm b} \rightarrow {\rm c^{+}}{\rm W^{-}}$ tree decay amplitude is one of the key goals of the LHCb experiment with first data. In the Standard Model (SM), this phase equals $-2\beta_s$, w...

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Autor principal: Conti, G
Lenguaje:eng
Publicado: 2009
Materias:
Acceso en línea:http://cds.cern.ch/record/1207119
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author Conti, G
author_facet Conti, G
author_sort Conti, G
collection CERN
description A measurement of the phase of the $\rm B_s$-$\bar{\rm B}_s$ oscillation amplitude with respect to that of the ${\rm b} \rightarrow {\rm c^{+}}{\rm W^{-}}$ tree decay amplitude is one of the key goals of the LHCb experiment with first data. In the Standard Model (SM), this phase equals $-2\beta_s$, which is predicted to be small, i.e. $\sim$-0.04 rad. Although the statistical uncertainties are large, the current results hint at a possible contribution of New Physics in the $\rm B_s$-$\bar{\rm B}_s$ box diagram. Already with 2 fb$^{-1}$ of data, corresponding to one nominal year of data taking, the LHCb experiment is expected to achieve a statistical uncertainty of $\sigma(2\beta_s)\simeq 0.03$ rad, similar to the $2\beta_s$ value predicted by the SM.
id cern-1207119
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2009
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spelling cern-12071192019-09-30T06:29:59Zhttp://cds.cern.ch/record/1207119engConti, G2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCbDetectors and Experimental TechniquesA measurement of the phase of the $\rm B_s$-$\bar{\rm B}_s$ oscillation amplitude with respect to that of the ${\rm b} \rightarrow {\rm c^{+}}{\rm W^{-}}$ tree decay amplitude is one of the key goals of the LHCb experiment with first data. In the Standard Model (SM), this phase equals $-2\beta_s$, which is predicted to be small, i.e. $\sim$-0.04 rad. Although the statistical uncertainties are large, the current results hint at a possible contribution of New Physics in the $\rm B_s$-$\bar{\rm B}_s$ box diagram. Already with 2 fb$^{-1}$ of data, corresponding to one nominal year of data taking, the LHCb experiment is expected to achieve a statistical uncertainty of $\sigma(2\beta_s)\simeq 0.03$ rad, similar to the $2\beta_s$ value predicted by the SM.LHCb-PROC-2009-033LHCb-CONF-2009-033CERN-LHCb-CONF-2009-033oai:cds.cern.ch:12071192009-09-17
spellingShingle Detectors and Experimental Techniques
Conti, G
2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title 2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title_full 2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title_fullStr 2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title_full_unstemmed 2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title_short 2$\beta_s$ measurement using B$_s^0$ $\rightarrow$ J$\psi\phi$ at LHCb
title_sort 2$\beta_s$ measurement using b$_s^0$ $\rightarrow$ j$\psi\phi$ at lhcb
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1207119
work_keys_str_mv AT contig 2betasmeasurementusingbs0rightarrowjpsiphiatlhcb