13 research outputs found

    Measurement of the CKM angle γ\gamma using B0DK0B^0 \rightarrow D K^{*0} with DKS0π+πD \rightarrow K^0_S \pi^+ \pi^- decays

    Get PDF
    A model-dependent amplitude analysis of the decay B0D(KS0π+π)K0B^0\rightarrow D(K^0_S\pi^+\pi^-) K^{*0} is performed using proton-proton collision data corresponding to an integrated luminosity of 3.0fb1^{-1}, recorded at s=7\sqrt{s}=7 and 8TeV8 TeV by the LHCb experiment. The CP violation observables x±x_{\pm} and y±y_{\pm}, sensitive to the CKM angle γ\gamma, are measured to be \begin{eqnarray*} x_- &=& -0.15 \pm 0.14 \pm 0.03 \pm 0.01, y_- &=& 0.25 \pm 0.15 \pm 0.06 \pm 0.01, x_+ &=& 0.05 \pm 0.24 \pm 0.04 \pm 0.01, y_+ &=& -0.65^{+0.24}_{-0.23} \pm 0.08 \pm 0.01, \end{eqnarray*} where the first uncertainties are statistical, the second systematic and the third arise from the uncertainty on the DKS0π+πD\rightarrow K^0_S \pi^+\pi^- amplitude model. These are the most precise measurements of these observables. They correspond to γ=(8022+21)\gamma=(80^{+21}_{-22})^{\circ} and rB0=0.39±0.13r_{B^0}=0.39\pm0.13, where rB0r_{B^0} is the magnitude of the ratio of the suppressed and favoured B0DK+πB^0\rightarrow D K^+ \pi^- decay amplitudes, in a KπK\pi mass region of ±50MeV\pm50 MeV around the K(892)0K^*(892)^0 mass and for an absolute value of the cosine of the K0K^{*0} decay angle larger than 0.40.4.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2016-007.htm

    Search for dark photons produced in 13 TeV pppp collisions

    Get PDF
    Searches are performed for both promptlike and long-lived dark photons, A 0 , produced in proton-proton collisions at a center-of-mass energy of 13 TeV, using A 0 → μ þ μ − decays and a data sample corresponding to an integrated luminosity of 1 . 6 fb − 1 collected with the LHCb detector. The promptlike A 0 search covers the mass range from near the dimuon threshold up to 70 GeV, while the long-lived A 0 search is restricted to the low-mass region 214 <m ð A 0 Þ < 350 MeV. No evidence for a signal is found, and 90% confidence level exclusion limits are placed on the γ – A 0 kinetic-mixing strength. The constraints placed on promptlike dark photons are the most stringent to date for the mass range 10 . 6 <m ð A 0 Þ < 70 GeV, and are comparable to the best existing limits for m ð A 0 Þ < 0 . 5 GeV. The search for long-lived dark photons is the first to achieve sensitivity using a displaced-vertex signature

    Erratum to: Measurements of the S-wave fraction in B-0 -> K+pi(-)mu(+)mu(-) decays and the B-0 -> K*(892)(0)mu(+)mu(-) differential branching fraction (vol 11, 047, 2016)

    No full text

    Measurement of the J/psi pair production cross-section in pp collisions at root s=13TeV

    No full text

    Measurements of CP asymmetries in charmless four-body Lambda(0)(b) and Xi(0)(b) decays

    No full text

    First observation of the decay D0Kπ+μ+μD^{0}\rightarrow K^{-}π^{+}μ^{+}μ^{-} in the ρ0ρ^{0}-ωω region of the dimuon mass spectrum

    No full text
    A study of the decay D0Kπ+μ+μD^{0}\rightarrow K^{-}\pi^{+}\mu^{+}\mu^{-} is performed using data collected by the LHCb detector in proton-proton collisions at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 2.0 fb1^{-1}. Decay candidates with muon pairs that have an invariant mass in the range 675--875 MeV/c2/c^2 are considered. This region is dominated by the ρ0\rho^{0} and ω\omega resonances. The branching fraction in this range is measured to be B{\cal B}(D0Kπ+μ+μD^{0}\rightarrow K^{-}\pi^{+}\mu^{+}\mu^{-} ) = (4.17±0.12(stat)±0.40(syst))×106( 4.17 \pm 0.12(stat) \pm 0.40(syst) )\times10^{-6}. This is the first observation of the decay D0Kπ+μ+μD^{0}\rightarrow K^{-}\pi^{+}\mu^{+}\mu^{-}. Its branching fraction is consistent with the value expected in the Standard Model

    Identification of beauty and charm quark jets at LHCb

    No full text
    Identification of jets originating from beauty and charm quarks is important for measuring Standard Model processes and for searching for new physics. The performance of algorithms developed to select b- and c-quark jets is measured using data recorded by LHCb from proton-proton collisions at root s = 7TeV in 2011 and at root s = 8TeV in 2012. The efficiency for identifying a b (c) jet is about 65%(25%) with a probability for misidentifying a light-parton jet of 0.3% for jets with transverse momentum pT > 20GeV and pseudorapidity 2 : 2 < eta < 4.2. The dependence of the performance on the pT and eta of the jet is also measured

    Search for Higgs-like bosons decaying into long-lived exotic particles

    Get PDF
    A search is presented for massive long-lived particles, in the 20–60&nbsp;GeV/c2 mass range with lifetimes between 5 and 100&nbsp;ps. The dataset used corresponds to 0.62fb-1 of proton-proton collision data collected by the LHCb detector at s=7TeV. The particles are assumed to be pair-produced by the decay of a Higgs-like boson with mass between 80 and 140&nbsp;GeV/c2. No excess above the background expectation is observed and limits are set on the production cross-section as a function of the long-lived particle mass and lifetime and of the Higgs-like boson mass

    B flavour tagging using charm decays at the LHCb experiment

    No full text
    An algorithm is described for tagging the flavour content at production of neutral B mesons in the LHCb experiment. The algorithm exploits the correlation of the flavour of a B meson with the charge of a reconstructed secondary charm hadron from the decay of the other b hadron produced in the proton-proton collision. Charm hadron candidates are identified in a number of fully or partially reconstructed Cabibbo-favoured decay modes. The algorithm is calibrated on the self-tagged decay modes B+ -> J/psi K+ and B-0 -> J/psi K*(0) using 3.0fb(-1) of data collected by the LHCb experiment at pp centre-of-mass energies of 7TeV and 8TeV. Its tagging power on these samples of B -> J/psi X decays is (0.30 +/- 0.01 +/- 0.01) %
    corecore