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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 â e±µâ 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 10â8 and 6.5 ·10â8, for B0d...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2007
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1028132 |
_version_ | 1780912316415475712 |
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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 â e±µâ 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 10â8 and 6.5 ·10â8, for B0d and B0s respectively, in 2 fbâ1. 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 |
record_format | invenio |
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 â e±µâ 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 10â8 and 6.5 ·10â8, for B0d and B0s respectively, in 2 fbâ1. 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 |