Bulletin of the American Physical Society
92nd Annual Meeting of the Southeastern Section of the APS
Thursday–Saturday, October 23–25, 2025; Festival Conference and Student Center, James Madison University, Harrisonburg, Virginia
Session J03: Nuclear and Particle Physics II
2:00 PM–3:36 PM,
Friday, October 24, 2025
James Madison University
Room: EnGeo1210
Chair: Aparajita Mazumdar, University of North Carolina at Chapel Hill
Abstract: J03.00005 : Precision Measurement of the R(D*) at the Belle II Experiment*
2:48 PM–3:00 PM
Presenter:
Romulus Godang
(University of South Alabama)
Author:
Romulus Godang
(University of South Alabama)
Br (anti-B0 → D*+ ℓ− anti-ν), where the lepton ℓ− denotes an electron or a muon.
The τ lepton is reconstructed in the leptonic decay of τ− → e− anti-νe ντ and τ− → μ− anti-νμ ντ.
The decay of anti-B0 → D*+ ℓ− anti-ν and anti-B0 → D*+ τ- anti-ν are reconstructed partially without reconstructing the intermediate decay of D0 meson. The semileptonic decay of anti-B0 → D*+ℓ−anti-ν is mediated by W boson. The W boson couples equally to the three lepton generations: e, μ, and τ. However, decays involving the τ lepton in the semitauonic decay of anti- B0 → D*+ τ− anti-ν provide a sensitive probe to additional amplitudes that involving an intermediate Higgs boson or a leptoquark being mediated in the transition of b → c τ ν. The partially reconstructed method may result in gain of as much as a factor 25 in statistics compared to the fully reconstructed method.
*This work was supported by the U.S. Department of Energy under grant No. DE-FOA-0002546
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