Abstract

The mixing-induced CP-violating phase ϕs in Bs0 and B¯s0 decays is measured using the J/ψπ+π− final state in data, taken from 3 fb−1 of integrated luminosity, collected with the LHCb detector in 7 and 8 TeV centre-of-mass pp collisions at the LHC. A time-dependent flavour-tagged amplitude analysis, allowing for direct CP violation, yields a value for the phase ϕs=70±68±8 mrad. This result is consistent with the Standard Model expectation and previous measurements.

Highlights

  • One of the most sensitive ways of detecting the presence of heretofore unseen particles or forces is through the observation of effects they may have on CP-violating decays of neutral B mesons [1]

  • The decay time distribution is influenced by acceptance effects that are introduced by track reconstruction, trigger and event selection

  • The CP phase φs is determined from the fit that uses the amplitude model with five final state π +π − resonances

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Summary

Introduction

One of the most sensitive ways of detecting the presence of heretofore unseen particles or forces is through the observation of effects they may have on CP-violating decays of neutral B mesons [1]. The complex parameters q and p are used to relate the mixing between the mass and flavour eigenstates. CP violation in the interference between mixing and decay associated with the state i, the amplitudes A and A can be further expressed as the sums of the individual. For J /ψ decays to μ+μ− final states, these amplitudes are themselves functions of four variables: the π +π − invariant mass mhh = m(π +π −), and the three angles Ω , defined in the helicity basis. These consist of the angle between the μ+ direction in the.

The LHCb detector and event selection
Likelihood construction
Decay time resolution and acceptance
Results
Systematic uncertainties
Conclusions
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