A study of B0s → ηc ϕ and B0s → ηc π+ π− decays is performed using pp collision data corresponding to an integrated luminosity of 3.0 fb^−1, collected with the LHCb detector in Run 1 of the LHC. The observation of the decay B0s → ηc ϕ is reported, where the ηc meson is reconstructed in the p anti-p, K+ K− π+ π−, π+ π− π+ π− and K+ K− K+ K− decay modes and the ϕ(1020) in the K+ K− decay mode. The decay B0s → J/ψ ϕ is used as a normalisation channel. Evidence is also reported for the decay B0s → ηc π+ π−, where the ηc meson is reconstructed in the p anti-p decay mode, using the decay B0s → J/ψ π+ π− as a normalisation channel. The measured branching fractions are B(B0s → ηc ϕ) = (5.01 ± 0.53 ± 0.27 ± 0.63) × 10^−4, B(B0s → ηc π+ π−) = (1.76 ± 0.59 ± 0.12 ± 0.29) × 10^−4, B(B0s → ηc ϕ) = (5.01 ± 0.53 ± 0.27 ± 0.63) × 10^−4, B(B0s → ηc π+ π−) = (1.76 ± 0.59 ± 0.12 ± 0.29) × 10^−4, where in each case the first uncertainty is statistical, the second systematic and the third uncertainty is due to the limited knowledge of the external branching fractions.
Observation of the Decay B0s → ηc ϕ and Evidence for B0s → ηc π+ π−
Capriotti, L.;
2017
Abstract
A study of B0s → ηc ϕ and B0s → ηc π+ π− decays is performed using pp collision data corresponding to an integrated luminosity of 3.0 fb^−1, collected with the LHCb detector in Run 1 of the LHC. The observation of the decay B0s → ηc ϕ is reported, where the ηc meson is reconstructed in the p anti-p, K+ K− π+ π−, π+ π− π+ π− and K+ K− K+ K− decay modes and the ϕ(1020) in the K+ K− decay mode. The decay B0s → J/ψ ϕ is used as a normalisation channel. Evidence is also reported for the decay B0s → ηc π+ π−, where the ηc meson is reconstructed in the p anti-p decay mode, using the decay B0s → J/ψ π+ π− as a normalisation channel. The measured branching fractions are B(B0s → ηc ϕ) = (5.01 ± 0.53 ± 0.27 ± 0.63) × 10^−4, B(B0s → ηc π+ π−) = (1.76 ± 0.59 ± 0.12 ± 0.29) × 10^−4, B(B0s → ηc ϕ) = (5.01 ± 0.53 ± 0.27 ± 0.63) × 10^−4, B(B0s → ηc π+ π−) = (1.76 ± 0.59 ± 0.12 ± 0.29) × 10^−4, where in each case the first uncertainty is statistical, the second systematic and the third uncertainty is due to the limited knowledge of the external branching fractions.| File | Dimensione | Formato | |
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2017-AR-40-Obs_of_the_Dec_B0s_to_etac_phi_and_Evid_for-JHEP.pdf
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