Study of the rare View the MathML sourceBs0 and B0B0 decays into the π+π−μ+μ−π+π−μ+μ− final state

A search for the rare decays B0 s → π +π −μ+μ− and B0 → π +π −μ+μ− is performed in a data set corresponding to an integrated luminosity of 3.0 fb−1 collected by the LHCb detector in proton- proton collisions at centre-of-mass energies of 7 and 8 TeV. Decay candidates with pion pairs that have invari...

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Detalles Bibliográficos
Autores: Garrido Beltrán, Lluís, Gascon, D., Graciani Díaz, Ricardo, Graugés Pous, Eugeni, Marin Benito, Carla, Picatoste Olloqui, Eduardo, Rives Molina, Vicente José, Ruiz, Hugo (Ruiz Pérez), LHCb Collaboration
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2015
País:España
Institución:Varias* (Consorci de Biblioteques Universitáries de Catalunya, Centre de Serveis Científics i Acadèmics de Catalunya)
Repositorio:Recercat. Dipósit de la Recerca de Catalunya
OAI Identifier:oai:recercat.cat:2445/185689
Acceso en línea:https://hdl.handle.net/2445/185689
Access Level:acceso abierto
Palabra clave:Hadrons
Gran Col·lisionador d'Hadrons
Física de partícules
Experiments
Large Hadron Collider (France and Switzerland)
Particle physics
Descripción
Sumario:A search for the rare decays B0 s → π +π −μ+μ− and B0 → π +π −μ+μ− is performed in a data set corresponding to an integrated luminosity of 3.0 fb−1 collected by the LHCb detector in proton- proton collisions at centre-of-mass energies of 7 and 8 TeV. Decay candidates with pion pairs that have invariant mass in the range 0.5-1.3 GeV/c2 and with muon pairs that do not originate from a resonance are considered. The first observation of the decay B0 s → π +π −μ+μ− and the first evidence of the decay B0 → π +π −μ+μ− are obtained and the branching fractions, restricted to the dipion-mass range considered, are measured to be B(B0 s → π +π −μ+μ−) = (8.6 ± 1.5 (stat) ± 0.7 (syst) ± 0.7 (norm)) × 10−8 and B(B0 → π +π −μ+μ−) = (2.11 ± 0.51 (stat) ± 0.15 (syst) ± 0.16 (norm)) × 10−8, where the third uncertainty is due to the branching fraction of the decay B0 → J /ψ(→ μ+μ−)K ∗(892)0(→ K +π −), used as a normalisation