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Observation of the Decay Λ_{b}^{0}→Λ_{c}^{+}τ^{-}ν[over ¯]_{τ}
R Aaij1, A S W Abdelmotteleb2, C Abellán Beteta3
1Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands.
Physical Review Letters
|May 27, 2022
Summary
The LHCb experiment observed the semileptonic b-baryon decay Lambda_b^0 to Lambda_c^+ tau^- nu, a significant finding in particle physics. This observation aligns with the Standard Model
Area of Science:
- Particle Physics
- High-Energy Physics
- B-Physics
Background:
- Semileptonic b-baryon decays are crucial for testing the Standard Model of particle physics.
- Previous studies have focused on decays involving lighter leptons, leaving the tau lepton channel less explored.
- The LHCb experiment at the Large Hadron Collider (LHC) provides a unique environment for studying such rare decays.
Purpose of the Study:
- To report the first observation of the semileptonic decay Lambda_b^0 -> Lambda_c^+ tau^- nu.
- To measure the branching fraction and ratios of this decay mode.
- To compare the results with Standard Model predictions and probe for potential new physics.
Main Methods:
- Analysis of a data sample corresponding to 3 fb^-1 of integrated luminosity collected by LHCb at 7 and 8 TeV.
- Reconstruction of the tau^- lepton through its hadronic decay channel (three charged pions).
- Measurement of branching fractions and ratios using a normalization channel (Lambda_b^0 -> Lambda_c^+ pi^- pi^+ pi^-).
Main Results:
- First observation of Lambda_b^0 -> Lambda_c^+ tau^- nu with a significance of 6.1 sigma.
- Measured branching fraction B(Lambda_b^0 -> Lambda_c^+ tau^- nu) = (1.50 +/- 0.16 +/- 0.25 +/- 0.23)%.
- Derived ratio of semileptonic branching fractions R(Lambda_c^+) = 0.242 +/- 0.026 +/- 0.040 +/- 0.059, consistent with the Standard Model.
Conclusions:
- The observation of this decay provides a new probe of b-baryon physics.
- The measured branching fractions and ratios are in agreement with the Standard Model predictions.
- This result contributes to the precise testing of the Standard Model in the heavy-quark sector.
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