A measurement of the $CP$-violating phase $\phi{_s}$ in the decay $B{^0_s} \to J/\psi\phi$

The LHCb experiment is dedicated to making precision measurements involving beauty and charm hadrons at the CERN Large Hadron Collider. The LHCb RICH detectors provide charged particle identification required to distinguish final states in many decays important to the LHCb physics programme. Time alignment of the RICH photon detectors is necessary in order to ensure a high photon collection efficiency. Using both a pulsed laser and proton-proton collision data the photon detectors are aligned to within 1~ns. The LHCb detector is uniquely positioned to measure production cross-sections at energies and rapidities inaccessible to other experiments. With 1.81~$\textrm{nb}^{-1}$~of proton-proton collisions collected by the LHCb experiment in 2010 at center-of-mass energy $\sqrt{s}=7~\textrm{TeV}$ the production cross-section of $D_{s}^{\pm}$ and $D^{\pm}$ mesons decaying to the $\phi\{K^{+}K^{-}\}\pi^{\pm}$ final state have been determined in bins of transverse momentum and rapidity. These measurements use a data-driven recursive optimisation technique to improve signal significance. The cross-section ratio is measured to be $\frac{\sigma(D^{\pm})}{\sigma(D_{s}^{\pm})} = 2.32\pm0.27\textrm{(stat)}\pm0.26\textrm{(syst)}$, consistent with the ratio of charm-quark hadronisation fractions to $D^{\pm}$ and $D_{s}^{\pm}$ mesons. Time-dependent interference between mixing of $B_{s}^{0}-{\bar B}_{s}^{0}$ mesons and decay to the final state $J/\psi\phi$ gives rise to a CP violating phase $\phi_s$. This phase is constrained to be small within the Standard Model, a significant deviation from which would be a signal of new physics. $\phi_{s}$ has been measured with 0.37~$\textrm{fb}^{-1}$~of proton-proton collision data recorded during 2011 by the LHCb experiment. Isolation of the signal distribution is achieved using the $\mathcal{S}\textrm{plot}$ technique, and the analysis accounts for inclusive $B_{s}^{0}\to J\psi K^{+}K^{-}$ s-wave contributions. The measured value of $\phi_{s}=0.16\pm 0.18 \textrm{(stat)}\pm0.06\textrm{(syst) rad}$ is the most precise measurement to date, and is consistent with Standard Model predictions.