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LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays

We discuss here the LHCb sensitivity to the B0d,s → e±µ∓ decays. These decays are forbidden in the Standard Model, being lepton flavor violating, but are allowed in some of its extensions. In absence of signal, we calculate the 90 % C.L. upper limits to be 1.6 10−8 and 6.5 ·10−8, for B0d...

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Detalles Bibliográficos
Autores principales: Bonivento, W, Serra, N
Lenguaje:eng
Publicado: 2007
Materias:
Acceso en línea:http://cds.cern.ch/record/1028132
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author Bonivento, W
Serra, N
author_facet Bonivento, W
Serra, N
author_sort Bonivento, W
collection CERN
description We discuss here the LHCb sensitivity to the B0d,s → e±µ∓ decays. These decays are forbidden in the Standard Model, being lepton flavor violating, but are allowed in some of its extensions. In absence of signal, we calculate the 90 % C.L. upper limits to be 1.6 10−8 and 6.5 ·10−8, for B0d and B0s respectively, in 2 fb−1. These results would improve the limits from present experiments. We discuss the interpretation of these results in the context of the Pati-Salam model, based on the group SU(4)C. This theory predicts the existence of a heavy spin-one gauge boson, the Pati-Salam Leptoquark which mediates the transitions between quarks and leptons. In this framework, the limits on branching fractions can be interpreted as lower limits on the Pati-Salam Leptoquark mass, which are 90·Fdmix TeV and 65·F smix TeV, at 90 % C.L., where the F d,smix are factors taking into account generation mixing within the Pati-Salam Mode.
id cern-1028132
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2007
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spelling cern-10281322019-09-30T06:29:59Zhttp://cds.cern.ch/record/1028132engBonivento, WSerra, NLHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decaysDetectors and Experimental TechniquesWe discuss here the LHCb sensitivity to the B0d,s → e±µ∓ decays. These decays are forbidden in the Standard Model, being lepton flavor violating, but are allowed in some of its extensions. In absence of signal, we calculate the 90 % C.L. upper limits to be 1.6 10−8 and 6.5 ·10−8, for B0d and B0s respectively, in 2 fb−1. These results would improve the limits from present experiments. We discuss the interpretation of these results in the context of the Pati-Salam model, based on the group SU(4)C. This theory predicts the existence of a heavy spin-one gauge boson, the Pati-Salam Leptoquark which mediates the transitions between quarks and leptons. In this framework, the limits on branching fractions can be interpreted as lower limits on the Pati-Salam Leptoquark mass, which are 90·Fdmix TeV and 65·F smix TeV, at 90 % C.L., where the F d,smix are factors taking into account generation mixing within the Pati-Salam Mode.LHCb-2007-028CERN-LHCb-2007-028oai:cds.cern.ch:10281322007-05-02
spellingShingle Detectors and Experimental Techniques
Bonivento, W
Serra, N
LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title_full LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title_fullStr LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title_full_unstemmed LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title_short LHCb sensitivity to the LFV B $B^0_{d,s}-> e\pm \mu\mp$ decays
title_sort lhcb sensitivity to the lfv b $b^0_{d,s}-> e\pm \mu\mp$ decays
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1028132
work_keys_str_mv AT boniventow lhcbsensitivitytothelfvbb0dsepmmumpdecays
AT serran lhcbsensitivitytothelfvbb0dsepmmumpdecays