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])
Name
PhysRevLett.115.111803.pdf
Size
507.29 KB
Format
Adobe PDF
Checksum (MD5)
403a3c7f466287c8aa5d2ffeb995e0c9
Author(s) •
Ilten, Philip J
Williams, Michael
Date Issued
September 2015
Journal
Physical Review Letters
Publisher
American Physical Society (APS)
Citation
Aaij, R., et al. “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])” Physical Review Letters, vol. 115, no. 11, Sept. 2015.
© 2015 CERN, for the LHCb Collaboration
Version
Final published version
Abstract
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.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Terms of Use
Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.
Persistent DSpace Link
DOI of Published Version
https://doi.org/10.1103/PHYSREVLETT.115.111803