Measurement of the Ratio of Branching Fractions B ([bar over B][superscript 0] → D[superscript * +] τ[superscript −] [bar over ν][subscript τ]) / B ([bar over B][supercript 0] → D[superscript * +]μ[superscript −][bar over ν][subscript μ])

• Main Authors: Ilten, Philip J (Contributor), Williams, Michael (Contributor)
• Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor), Massachusetts Institute of Technology. Laboratory for Nuclear Science (Contributor)
• Format: Article
• Language: English
• Published: American Physical Society (APS), 2018-05-30T13:41:56Z.
• Subjects: Article
• Online Access: Get fulltext

The branching fraction ratio R(D[superscript ∗])≡B([bar over B][superscript 0]→D[superscript ∗+]τ[superscript -][bar overν][subscript τ])/B([bar over B][superscript 0]→D[superscript ∗+]μ[superscript -][bar over ν][subscript μ]) is measured using a sample of proton-proton collision data corresponding to 3.0fb[supercript -1] of integrated luminosity recorded by the LHCb experiment during 2011 and 2012. The tau lepton is identified in the decay mode τ-→μ[superscript -][bar over ν][subscript μ]ν[subscript τ]. The semitauonic decay is sensitive to contributions from non-standard-model particles that preferentially couple to the third generation of fermions, in particular, Higgs-like charged scalars. A multidimensional fit to kinematic distributions of the candidate [bar overB][subscript 0] decays gives R(D[superscript ∗]) = 0.336 ± 0.027(stat) ± 0.030(syst). This result, which is the first measurement of this quantity at a hadron collider, is 2.1 standard deviations larger than the value expected from lepton universality in the standard model.
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