154 research outputs found

    Inclusive V0V^0 Production Cross Sections from 920 GeV Fixed Target Proton-Nucleus Collisions

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    Inclusive differential cross sections dσpA/dxFd\sigma_{pA}/dx_F and dσpA/dpt2d\sigma_{pA}/dp_t^2 for the production of \kzeros, \lambdazero, and \antilambda particles are measured at HERA in proton-induced reactions on C, Al, Ti, and W targets. The incident beam energy is 920 GeV, corresponding to s=41.6\sqrt {s} = 41.6 GeV in the proton-nucleon system. The ratios of differential cross sections \rklpa and \rllpa are measured to be 6.2±0.56.2\pm 0.5 and 0.66±0.070.66\pm 0.07, respectively, for \xf 0.06\approx-0.06. No significant dependence upon the target material is observed. Within errors, the slopes of the transverse momentum distributions dσpA/dpt2d\sigma_{pA}/dp_t^2 also show no significant dependence upon the target material. The dependence of the extrapolated total cross sections σpA\sigma_{pA} on the atomic mass AA of the target material is discussed, and the deduced cross sections per nucleon σpN\sigma_{pN} are compared with results obtained at other energies.Comment: 17 pages, 7 figures, 5 table

    Observation of charmless hadronic B decays

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    Four candidates for charmless hadronic B decay are observed in a data sample of four million hadronic Z decays recorded by the ALEPH detector at LEP. The probability that these events come from background sources is estimated to be less than 10(-6). The average branching of weakly decaying B hadrons (a mixture of B-d(0), B-s(0) and Lambda(b) weighted by their production The average branching ratio of weakly decaying B hadrons (a mixture of B-d(0) cross sections and lifetimes, here denoted B) into two long-lived charged hadrons (pions, kaons or protons) is measured to be Br(B-->h(+)h(-))=(1.7(-0.7)(+1.0)+/-0.2)x10(-5). The relative branching fraction Br(B-d(s)(0)-->pi(+)pi(-)(K-))/Br(B-d(s)(0)-->h(+)h(-)) is measured to be 1.0(-0.3-0.1)(+0.0+0.0). In addition, branching ratio upper limits are obtained for a variety of exclusive charmless hadronic two-body decays of B hadrons

    Higgs at ATLAS

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    A review of the ATLAS results for Higgs to WW, gamma gamma, tau tau and ZZ is given with the present analysis of couplings, spin and mass. This is to be presented at the 16th Lomonosov conference

    Higgs Boson Physics at ATLAS

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    The discovery of a new boson with the ATLAS detector at the LHC proton-proton collider is confirmed using the full data set collected at centre-of-mass energies of 7 and 8 TeV. The spin and parity properties of the boson are consistent with that of a scalar particle with positive parity. Comparison of the JP=0+J^{P}=0^+ hypothesis to alternatives JP=0,1+,1,2+J^{P} = 0^-,1^{+},1^-,2^+ result in exclusion of these other choices at 97.8\%, 99.97\%, 99.7\%, and 99.3\% CL. The Higgs-boson Mass is mH=125.5±0.2(stat.)0.5+0.5(syst.)m_H = 125.5 \pm 0.2 {\rm (stat.)} ^{+0.5}_{-0.5} {\rm (syst.)} \GeV. Evidence for production of the Higgs boson by vector boson fusion is obtained in a model-independent approach by comparing the signal strengths μ\mu of vector boson fusion and production associated with a vector boson to to that for gluon fusion including associated production of top quark pairs: μVBF+VH/μggF+ttH=1.40.3+0.4(stat.)0.4+0.6(syst.)\mu_{\rm VBF+VH}/\mu_{\rm ggF+ttH}= 1.4 ^{+0.4}_{-0.3} \rm{(stat.)} ^{+0.6}_{-0.4} \rm{(syst.)} which is 3.3 Gaussian standard deviations from zero

    Ks0 Production In Pbarp Interactions At Square-root-of-s=630 and 1800 Gev

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    Jet-fragmentation Properties In Pbarp Collisions At Square-root-s = 1.8 Tev

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    Search For Heavy Stable Charged-particles In 1.8-tev Ppbar Collisions At the Fermilab Collider

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