Evidence for the decay X(3872)→ψ(2S)γ
Nuclear Physics B 886 (2014) 665-680
Abstract:
Evidence for the decay mode X(3872)→ψ(2S)γ in B +→X(3872)K + decays is found with a significance of 4.4 standard deviations. The analysis is based on a data sample of proton-proton collisions, corresponding to an integrated luminosity of 3 fb-1, collected with the LHCb detector, at centre-of-mass energies of 7 and 8 TeV. The ratio of the branching fraction of the X(3872)→ψ(2S)γ decay to that of the X(3872)→J/ψγ decay is measured to beB(X(3872)→ψ(2S)γ)B(X(3872)→J/ψγ)=2.46±0.64±0.29, where the first uncertainty is statistical and the second is systematic. The measured value does not support a pure DD-* molecular interpretation of the X(3872) state. © 2014 CERN for the benefit of the LHCb Collaboration.Measurement of CP asymmetries in the decays B0 → K*0μ+μ− and B+ → K+μ+μ−
Journal of High Energy Physics 2014:9 (2014) 1-18
Abstract:
© 2014, The Author(s). Abstract: The direct CP asymmetries of the decays B0 → K*0μ+μ− and B+ → K+μ+μ− are measured using pp collision data corresponding to an integrated luminosity of 3.0 fb−1 collected with the LHCb detector. The respective control modes B0 → J/ψK*0 and B+ → J/ψK+ are used to account for detection and production asymmetries. The measurements are made in several intervals of μ+μ− invariant mass squared, with the ϕ(1020) and charmonium resonance regions excluded. Under the hypothesis of zero CP asymmetry in the control modes, the average values of the asymmetries are (Formula Presented)where the first uncertainties are statistical and the second are due to systematic effects. Both measurements are consistent with the Standard Model prediction of small CP asymmetry in these decays.[Figure not available: see fulltext.]Measurement of CP asymmetries in the decays B0→ K*0μ+μ−and B+→ K+μ+μ−
Journal of High Energy Physics 2014:9 (2014)
Abstract:
The direct CP asymmetries of the decays B0→ K*0μ+μ−and B+→ K+μ+μ−are measured using pp collision data corresponding to an integrated luminosity of 3.0 fb−1collected with the LHCb detector. The respective control modes B0→ J/ψK*0and B+→ J/ψK+are used to account for detection and production asymmetries. The measurements are made in several intervals of μ+μ−invariant mass squared, with the ϕ(1020) and charmonium resonance regions excluded. Under the hypothesis of zero CP asymmetry in the control modes, the average values of the asymmetries are (Formula Presented) where the first uncertainties are statistical and the second are due to systematic effects. Both measurements are consistent with the Standard Model prediction of small CP asymmetry in these decays.Measurement of cp asymmetries in the decays b0 → k*0μ+μ- and b+ → k+μ+μ-
Journal of High Energy Physics 2014:177 (2014)
Abstract:
The direct CP asymmetries of the decays B0 → K*0μ+μ- and B+ → K+μ+μ- are measured using pp collision data corresponding to an integrated luminosity of 3.0 fb-1 collected with the LHCb detector. The respective control modes B0 → J/ψK*0 and B+ → J/ J/ψK+ are used to account for detection and production asymmetries. The measurements are made in several intervals of μ+μ- invariant mass squared, with the Ф(1020) and charmonium resonance regions excluded. Under the hypothesis of zero CP asymmetry in the control modes, the average values of the asymmetries are where the first uncertainties are statistical and the second are due to systematic effects. Both measurements are consistent with the Standard Model prediction of small CP asymmetry in these decays.Measurement of polarization amplitudes and cp asymmetries in B0 → φK∗(892)0
Journal of High Energy Physics 2014:5 (2014)