22 research outputs found

    Forward production of Υ\Upsilon mesons in pppp collisions at s=7\sqrt{s}=7 and 8TeV

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    The production of Υ\Upsilon mesons in pppp collisions at =7\sqrt=7 and 8 TeV8\,\mathrm{TeV} is studied with the LHCb detector using data samples corresponding to an integrated luminosity of 1 fb−11\,\mathrm{fb}^{-1} and 2 fb−12\,\mathrm{fb}^{-1} respectively. The production cross-sections and ratios of cross-sections are measured as functions of the meson transverse momentum pTp_T and rapidity yy, for pT<30 GeV/cp_T<30\,\mathrm{GeV}/c} and 2.0<y<4.52.0<y<4.5.Comment: 36 pages, 7 figures, 16 tables. 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-2015-045.htm

    Observation of the decay Bc+ B_c^{+} → J/ψ K + K − π +

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    Measurement of the ratio of the production cross sections times branching fractions of B c ±  → J/ψπ ± and B± → J/ψK ± and ℬ B c ± → J / ψ π ± π ± π ∓ / ℬ B c ± → J / ψ π ± B(Bc±→J/ψπ±π±π∓)/B(Bc±→J/ψπ±) \mathrm{\mathcal{B}}\left({\mathrm{B}}_{\mathrm{c}}^{\pm}\to \mathrm{J}/\psi {\pi}^{\pm }{\pi}^{\pm }{\pi}^{\mp}\right)/\mathrm{\mathcal{B}}\left({\mathrm{B}}_{\mathrm{c}}^{\pm}\to \mathrm{J}/\psi {\pi}^{\pm}\right) in pp collisions at s = 7 s=7 \sqrt{s}=7 TeV

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    Associated production of a quarkonium and a Z boson at one loop in a quark-hadron-duality approach

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    22 pages, 9 figures, 3 tables. LaTeX uses jheppub.styInternational audienceIn view of the large discrepancy about the associated production of a prompt J/ψJ/\psi and a ZZ boson between the ATLAS data at s=8\sqrt{s}=8 TeV and theoretical predictions for Single Parton Scattering (SPS) contributions, we perform an evaluation of the corresponding cross section at one loop accuracy (Next-to-Leading Order, NLO) in a quark-hadron-duality approach, also known as the Colour-Evaporation Model (CEM). This work is motivated by (i) the extremely disparate predictions based on the existing NRQCD fits conjugated with the absence of a full NLO NRQCD computation and (ii) the fact that we believe that such an evaluation provides a likely upper limit of the SPS cross section. In addition to these theory improvements, we argue that the ATLAS estimation of the Double Parton Scattering (DPS) yield may be underestimated by a factor as large as 3 which then reduces the size of the SPS yield extracted from the ATLAS data. Our NLO SPS evaluation also allows us to set an upper limit on σeff\sigma_{\rm eff} driving the size of the DPS yield. Overall, the discrepancy between theory and experiment may be smaller than expected, which calls for further analyses by ATLAS and CMS, for which we provide predictions, and for full NLO computations in other models. As an interesting side product of our analysis, we have performed the first NLO computation of dσ/dPTd\sigma / dP_T for prompt single-J/ψJ/\psi production in the CEM from which we have fit the CEM non-pertubative parameter at NLO using the most recent ATLAS data
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