Measurement of the Ratio of the B0→D*−τ+ντ and B0→D*−μ+νμ Branching Fractions Using Three-Prong τ-Lepton Decays

dc.contributor.author
Alfonso Albero, Alejandro
dc.contributor.author
Badalov, Alexey
dc.contributor.author
Calvo Gómez, Míriam
dc.contributor.author
Camboni, Alessandro
dc.contributor.author
Coquereau, Samuel
dc.contributor.author
Fernandez, G.
dc.contributor.author
Garrido Beltrán, Lluís
dc.contributor.author
Gascón Fora, David
dc.contributor.author
Graciani Díaz, Ricardo
dc.contributor.author
Graugés Pous, Eugeni
dc.contributor.author
Marin Benito, Carla
dc.contributor.author
Picatoste Olloqui, Eduardo
dc.contributor.author
Rives Molina, Vicente José
dc.contributor.author
Vilasis-Cardona, Xavier
dc.contributor.author
LHCb Collaboration
dc.date.issued
2019-04-29T09:57:22Z
dc.date.issued
2019-04-29T09:57:22Z
dc.date.issued
2018-04-25
dc.date.issued
2019-04-29T09:57:23Z
dc.identifier
0031-9007
dc.identifier
https://hdl.handle.net/2445/132497
dc.identifier
684704
dc.description.abstract
The ratio of branching fractions R ( D * − ) ≡ B ( B 0 → D * − τ + ν τ ) / B ( B 0 → D * − μ + ν μ ) is measured using a data sample of proton-proton collisions collected with the LHCb detector at center-of-mass energies of 7 and 8 TeV, corresponding to an integrated luminosity of 3     fb − 1 . For the first time, R ( D * − ) is determined using the τ -lepton decays with three charged pions in the final state. The B 0 → D * − τ + ν τ yield is normalized to that of the B 0 → D * − π + π − π + mode, providing a measurement of B ( B 0 → D * − τ + ν τ ) / B ( B 0 → D * − π + π − π + ) = 1.97 ± 0.13 ± 0.18 , where the first uncertainty is statistical and the second systematic. The value of B ( B 0 → D * − τ + ν τ ) = ( 1.42 ± 0.094 ± 0.129 ± 0.054 ) % is obtained, where the third uncertainty is due to the limited knowledge of the branching fraction of the normalization mode. Using the well-measured branching fraction of the B 0 → D * − μ + ν μ decay, a value of R ( D * − ) = 0.291 ± 0.019 ± 0.026 ± 0.013 is established, where the third uncertainty is due to the limited knowledge of the branching fractions of the normalization and B 0 → D * − μ + ν μ modes. This measurement is in agreement with the standard model prediction and with previous results.
dc.format
11 p.
dc.format
application/pdf
dc.language
eng
dc.publisher
American Physical Society
dc.relation
Reproducció del document publicat a: https://doi.org/10.1103/PhysRevLett.120.171802
dc.relation
Physical Review Letters, 2018, vol. 120, num. 17, p. 171802
dc.relation
https://doi.org/10.1103/PhysRevLett.120.171802
dc.rights
cc by (c) CERN; LHCb Collaboration, 2018
dc.rights
http://creativecommons.org/licenses/by/3.0/es/
dc.rights
info:eu-repo/semantics/openAccess
dc.source
Articles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject
Física de partícules
dc.subject
Experiments
dc.subject
Particle physics
dc.subject
Experiments
dc.title
Measurement of the Ratio of the B0→D*−τ+ντ and B0→D*−μ+νμ Branching Fractions Using Three-Prong τ-Lepton Decays
dc.type
info:eu-repo/semantics/article
dc.type
info:eu-repo/semantics/publishedVersion


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