150 research outputs found

    Charged rho meson production in neutrino-induced reactions at E_nu = 10 GeV

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    The neutrinoproduction of charged ρ\rho mesons on nuclei and nucleons is investigated for the first time at moderate energies ( \approx 10 GeV), using the date obtained with SKAT bubble chamber. No strong nuclear effects are observed in ρ+\rho^+ and ρ\rho^- production. The fractions of charged and neutral pions originating from ρ\rho decays are obtained and compared with higher energy data. From analysis of the obtained and available data on ρ+\rho^+ and K+K^{*+}(892) neutrinoproduction, the strangeness suppression factor in the quark string fragmentation is extracted: λs=0.18±0.03\lambda_s = 0.18\pm0.03. Estimations are obtained for cross sections of quasiexclusive single ρ+\rho^+ and coherent ρ+\rho^+ neutrinoproduction on nuclei. The estimated coherent cross section σρ+coh\sigma_{\rho^+}^{coh} = (0.29±0.16)1038\pm0.16)\cdot 10^{-38} cm2^2 is compatible with theoretical predictions.Comment: 7 pages, 6 figure

    A study of the double hadron neutrinoproduction on nuclei

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    The nuclear medium influence on the dihadron neutrinoproduction is investigated for the first time, using the data obtained with SKAT bubble chamber. An indication is obtained that the nuclear attenuation of the dihadron is more expressed for kinematically closest hadron pairs. The experimental data on the dihadron attenuation and on the ratio of the dihadron to single-hadron yields are compared with predictions of the two-scale string fragmentation model.Comment: 5 pages, 10 figure

    Charm and bottom production in inclusive double Pomeron exchange in heavy ion collisions at the LHC

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    The inclusive double Pomeron exchange cross section for heavy quark pair production is calculated for nucleus-nucleus collisions at the LHC. The present estimate is based on hard diffractive factorization, corrected by absorptive corrections and nuclear effects. The theoretical uncertainties for nuclear collisions are investigated and a comparison to other approaches is presented. The production channels producing a similar final state configuration are discussed as well.Comment: 7 pages, 3 tables. Final version to be published in Physical Review

    Coherent and Non-Coherent Double Diffractive Production of QQˉ Q \bar {Q} - pairs in Collisions of Heavy Ions at High Energies

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    The double coherent and non-coherent diffractive production of heavy quark - antiquark pairs (QQˉQ \bar{Q}) in heavy ion scattering at high energies (LHC) is considered. The total and differential cross sections of these processes with the formation of ccˉc \bar{c} and bbˉb \bar{b} pairs in pppp, CaCaCaCa and PbPbPbPb collisions are evaluated. The contribution of the considered mechanisms is a few per cent of the number of heavy quark - antiquark pairs obtained in the processes of hard (QCD) scattering, and it will be taken into account in the registration of cc, bb quarks or, for instance, in the study of the heavy quarkonia suppression effects in Quark - Gluon Plasma, in the search for intermediate mass Higgs bosons and so on. It is shown that the cross section of the coherent scattering process is great enough. This makes it suitable for studying collective effects in nuclear interactions at high energies. An example of such effects is given: large values of the invariant mass of a QQˉQ \bar{Q}pair, M_{Q \bar{Q}} \gsim 100 GeV, in association with a large rapidity gap between diffractive jets Δη>5\Delta \eta > 5.Comment: 22 pages, 5(.eps) figures, 3 tables, LaTe

    The yields of light meson resonances in neutrinonuclear interactions at <E_nu> = 10 GeV

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    The total yields of the all well-established light mesonic resonances (up to the ϕ\phi(1020) meson) are estimated in neutrinonuclear interactions at < E_nu > = 10 GeV, using the data obtained with SKAT bubble chamber. For some resonances, the yields in the forward and backward hemispheres in the hadronic c.m.s. are also extracted. From the comparison of the obtained and available higher-energy data, an indication is obtained that the resonance yields rise almost linearly as a function of the mean mass of the neutrinoproduced hadronic system. The fractions of pions originating from the light resonance decays are inferred.Comment: 15 pages, 7 figure
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