Measurement of the effective Bs0→K+K- lifetime
Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics 707:3-4 (2012) 349-356
Abstract:
A measurement of the effective Bs0→K+K- lifetime is presented using approximately 37pb-1 of data collected by LHCb during 2010. This quantity can be used to put constraints on contributions from processes beyond the Standard Model in the Bs0 meson system and is determined by two complementary approaches asτKK=1.440±0.096(stat)±0.008(syst)±0.003(model)ps. © 2011 CERN.Observation of J/ψ-pair production in pp collisions at √s=7 TeV
Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics 707:1 (2012) 52-59
Abstract:
The production of J/ψ pairs in proton-proton collisions at a centre-of-mass energy of 7 TeV has been observed using an integrated luminosity of 37.5 pb -1 collected with the LHCb detector. The production cross-section for pairs with both J/ψ in the rapidity range 2Inclusive W and Z production in the forward region at √ s = 7 TeV
Journal of High Energy Physics 2012:6 (2012)
Abstract:
Measurements of inclusive W and Z boson production cross-sections in pp collisions at √ s = 7TeV using final states containing muons are presented. The data sample corresponds to an integrated luminosity of 37 pb -1 collected with the LHCb detector. The W and Z bosons are reconstructed from muons with a transverse momentum above 20 GeV/c and pseudorapidity between 2:0 and 4:5, and, in the case of the Z cross-section, a dimuon invariant mass between 60 and 120 GeV/c2. The cross-sections are measured to be 831±9±27±29 pb for W+, 656±8±19±23 for W- and 76:7±1:7±3: 3±2:7 pb for Z, where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity. Differential cross-sections, W and Z cross-section ratios and the lepton charge asymmetry are also measured in the same kinematic region. The ratios are determined to be σW+→μ+ν/σW- →μ-ν = 1:27±0:02±0:01 and ( σW+→μ+ν+σW- →μ-ν)/σZ→μμ = 19:4±0:5± 0:9. The results are in general agreement with theoretical predictions, performed at nextto- next-to-leading order in QCD using recently calculated parton distribution functions. Copyright CERN.Measurement of b-hadron branching fractions for two-body decays into charmless charged hadrons
Journal of High Energy Physics 2012:10 (2012)
Abstract:
Based on data corresponding to an integrated luminosity of 0.37 fb -1 collected by the LHCb experiment in 2011, the following ratios of branching fractions are measured: B(B0 → π+π -) / B(B0 → K+π-) = 0.262 ± 0.009 ± 0.017; (fs/fd) B(Bs0 → K +K-) / B(B0 → K+π -) = 0.316 ± 0.009 ± 0.019; (fs/fd) B(B s0 → π+K-) / B(B0 → K+π-) = 0.074 ± 0.006 ± 0.006; (fd/fs) ± B(B0 → K+K-) / B(B s0 → K+K-) = 0.018 -0.007 +-0.007 ± 0.009; (fs/fd) B(Bs0 → π+π-) / B(B0 → π+π-) = 0.050 -0.009+0.011 ± 0.004; BΛb0 → pπ-) / BΛb0 → pK-) = 0.86 ± 0.08 ± 0.05; where the πrst uncertainties are statistical and the second systematic. Using the current world average of B(B0 → K +π-π and the ratio of the strange to light neutral B meson production fs/fd measured by LHCb, we obtain: B(B0 → π+π-) = (5.08 ± 0.17 ± 0.37) × 10-6; B(Bs0 → K+K-) = (23.0 ± 0.7 ± 2.3) × 10-6; B(Bs0 → π+K-) = (5.4 ± 0.4 ± 0.6) × 10-6; B(B0 → K+K-) = (0.11 -0.04+0.05 ± 0.06) × 10 -6; B(Bs0 → π+π -) = (0.95 -0.17+0.21 ± 0.13) × 10-6. The measurements of B(Bs0 → K +K-), B(Bs0 → π+K-) and B(B0 → K+K -) are the most precise to date. The decay mode Bs0 → π+π- is observed for the first time with a significance of more than 5σ. Copyright CERN.Measurement of charged particle multiplicities in pp collisions at √s = 7 TeV in the forward region
European Physical Journal C 72:4 (2012)