Measurement of the τ−→ηπ−π+π−ντ branching fraction and a search for a second-class current in the τ−→η′(958)π−ντ decay

The τ − → η π − π + π − ν τ decay with the η → γ γ mode is studied using 384     fb − 1 of data collected by the BABAR detector. The branching fraction is measured to be ( 1.60 ± 0.05 ± 0.11 ) × 10 − 4 . It is found that τ − → f 1 ( 1285 ) π − ν τ → η π − π + π − ν τ is the dominant decay mode with...

Descripción completa

Detalles Bibliográficos
Autores: Garra Ticó, Jordi, Graugés Pous, Eugeni, BABAR Collaboration
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2008
País:España
Institución:Universidad de Barcelona
Repositorio:Dipòsit Digital de la UB
OAI Identifier:oai:diposit.ub.edu:2445/131523
Acceso en línea:https://hdl.handle.net/2445/131523
Access Level:acceso abierto
Palabra clave:Física de partícules
Experiments
Particle physics
Descripción
Sumario:The τ − → η π − π + π − ν τ decay with the η → γ γ mode is studied using 384     fb − 1 of data collected by the BABAR detector. The branching fraction is measured to be ( 1.60 ± 0.05 ± 0.11 ) × 10 − 4 . It is found that τ − → f 1 ( 1285 ) π − ν τ → η π − π + π − ν τ is the dominant decay mode with a branching fraction of ( 1.11 ± 0.06 ± 0.05 ) × 10 − 4 . The first error on the branching fractions is statistical and the second systematic. Note that no particle identification algorithm is applied to the charged tracks to distinguish pions from kaons. In addition, a 90% confidence level upper limit on the branching fraction of the τ − → η ′ ( 958 ) π − ν τ decay is measured to be 7.2 × 10 − 6 . This last decay proceeds through a second-class current and is expected to be forbidden in the limit of isospin symmetry.