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  1. No Access

    Article

    Differential cross sections of proton compton scattering at photon laboratory energies between 700 and 1000 MeV

    Differential cross sections of proton Compton scattering have been measured at the Bonn 2.5 GeV synchrotron. 78 data points are presented as angular distributions at photon lab energies of 700, 750, 800, 850, ...

    M. Jung, J. Kattein, H. Kück, P. Leu in Zeitschrift für Physik C Particles and Fie… (1981)

  2. No Access

    Article

    Further evidence for photoproduction of charmedF-mesons

    Further experimental evidence is given for theF meson through its decay into η′s. Results are presented for the decay channels ηπ±, ηπ0π± and ηπ+ππ±, and confirm those obtained in a previous experiment.

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1983)

  3. No Access

    Article

    Differential cross sections of proton compton scattering at photon laboratory energies between 1.2 and 1.7 GeV

    Differential cross sections of proton Compton scattering have been measured at the Bonn 2.5 GeV synchrotron. The experiment covers photon laboratory energies between 1.2 GeV and 1.7 GeV and the square of the f...

    J. Duda, F. -W. Höfner, M. Jung in Zeitschrift für Physik C Particles and Fie… (1983)

  4. No Access

    Article

    Photoproduction of multiparticle states in the beam fragmentation region for photon energies in the range 50–70 GeV

    Forward production of hadrons in γp interactions at about 11 GeV centre of mass energy has been analysed in terms of single particle spectra. Comparisons withK + p andK p data and with deep inelastic scattering...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1984)

  5. No Access

    Article

    Photoproduction of ϕ mesons by linearly polarized photons of energy 20–40 GeV and further evidence for a photoproduced high-massKK enhancement

    A study of ϕ-meson photoproduction by partially polarized photons of energy 20–40 GeV is reported. The production mechanism is found to conserves-channel helicity and to proceed via natural-parity exchange in the

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1985)

  6. No Access

    Article

    Evidence for a ωϱ±π± state in diffractive photoproduction

    The photoproduction of the final state ω π+ππ0 has been studied as part of a survey of photoproduction in the energy range 20–70 GeV in the Omega spectrometer at CERN. The π+ππ0 system produced with the ω meson...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1985)

  7. No Access

    Article

    The ρ′ in the reaction γp→ π+ππ0π0 p at photon energies of 20–70 GeV

    The reactionγpπ + π π 0 π 0 p (excludingωπ 0 production) has been studied for photon energies in the range 20–70 GeV. A peak is seen in the 4π mass spectrum at ∼1.66 GeV with a width of ∼0.3 GeV which is ident...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1985)

  8. No Access

    Article

    Study ofηπ+π in the ϱ′(1600) mass region photoproduced in the reaction γpηπ+π p at photon energies of 20 to 70 GeV

    In diffractive photoproduction ofηπ+π, the two-body substatesηρ0 andA 2π are found to contribute significantly to the cross-section forηπ+π masses below 2.4 GeV. From a spin-parity analysis the branching ratio,...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1986)

  9. No Access

    Article

    Search for a ϕ′ vector meson in diffractive photoproduction ofK + K π+π

    A study of photoproduction ofK + K π+π shows a broad threshold enhancement, about 30% of which is due toK * Kπ production. ThisK * Kπ component shows no dynamical features indicative of the existence of a ϕ′ ve...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1986)

  10. No Access

    Article

    Inclusive photoproduction of ϕ,K *(890) andK *(1420) in the photon energy range 20 to 70 GeV

    Inclusive photoproduction of ϕ,K *0(890), \(\bar K*^0 \) andK *0(1420),

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1986)

  11. No Access

    Article

    Diffractive photoproduction of ab 1π system

    It is shown that a likely interpretation of theb 1 ± π mass spectrum from diffractive photoproduction is that it is due to contributions from the ω3(1670), i...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1987)

  12. No Access

    Article

    A peak in the η ω mass spectrum from diffractive photoproduction

    The η ω mass spectrum resulting from diffractive photoproduction, by photons of 25–50 GeV, shows a peak at a mass of 1.61±0.04 GeV and width of 0.23±0.08 GeV. Comparison with the corresponding η ρ0 mass spectrum ...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1987)

  13. No Access

    Article

    Photon diffractive dissociation to ρρπ and ρπππ states

    This paper reports studies of the reactions γp→ρ π π πp and γp→ρ ρ πp. In particular a peak is reported in the ρ ρ π mass spectrum with closely similar mass and width to those of the ω ρ π peak previously reporte...

    M. Atkinson, T. J. Axon, D. Barberis in Zeitschrift für Physik C Particles and Fie… (1988)

  14. Article

    Open Access

    Implications of LHCb measurements and future prospects

    During 2011 the LHCb experiment at CERN collected 1.0 fb−1 of \(\sqrt{s} = 7\mbox{~TeV}\) pp collisions. ...

    A. Bharucha, I. I. Bigi, C. Bobeth, M. Bobrowski in The European Physical Journal C (2013)

  15. Article

    Open Access

    The phenomenology of electric dipole moments in models of scalar leptoquarks

    We study the phenomenology of electric dipole moments (EDMs) induced in various scalar leptoquark models. We consider generic leptoquark couplings to quarks and leptons and match to Standard Model effective fi...

    W. Dekens, J. de Vries, M. Jung, K. K. Vos in Journal of High Energy Physics (2019)

  16. Article

    Open Access

    Measurement of electrons from heavy-flavour hadron decays as a function of multiplicity in p-Pb collisions at \( \sqrt{s_{\mathrm{NN}}} \) = 5.02 TeV

    The multiplicity dependence of electron production from heavy-flavour hadron decays as a function of transverse momentum was measured in p-Pb collisions at ...

    S. Acharya, D. Adamová, S. P. Adhya, A. Adler in Journal of High Energy Physics (2020)

  17. Article

    Open Access

    Underlying event properties in pp collisions at \( \sqrt{s} \) = 13 TeV

    This article reports measurements characterizing the Underlying Event (UE) associated with hard scatterings at midrapidity (|η| < 0.8) in pp collisions at s\( \sqrt{s} \) = 13 TeV. The hard scatterings are identi...

    S. Acharya, D. Adamová, A. Adler, J. Adolfsson in Journal of High Energy Physics (2020)

  18. Article

    Open Access

    Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at \( \sqrt{s_{\mathrm{NN}}} \) = 5.02 TeV

    Anisotropic flow coefficients, vn, non-linear flow mode coefficients, χn,mk, and correlations among different symmetry planes, ρn,mk are measured in Pb-Pb collisions at s NN \( \sqrt{s_{\mathrm{NN}}} \) =...

    S. Acharya, D. Adamová, A. Adler, J. Adolfsson in Journal of High Energy Physics (2020)

  19. Article

    Open Access

    Coherent photoproduction of ρ0 vector mesons in ultra-peripheral Pb-Pb collisions at \( \sqrt{{\mathrm{s}}_{\mathrm{NN}}} \) = 5.02 TeV

    Cross sections for the coherent photoproduction of ρ0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN \( \sqrt{{\mathrm{s}}_{\mathrm{NN}}} \) = 5.02 TeV are reported. The measurements, which re...

    S. Acharya, D. Adamová, A. Adler, J. Adolfsson in Journal of High Energy Physics (2020)

  20. Article

    Open Access

    Non-linear flow modes of identified particles in Pb-Pb collisions at \( \sqrt{s_{\mathrm{NN}}} \) = 5.02 TeV

    The pT-differential non-linear flow modes, v4,22, v5,32, v6,33 and v6,222 for π±, K±, K S 0 \( {\mathrm{K}}_{\mathrm{S}}^0 \) , p + p ¯ \( \overline{\mathrm{p}} \) , Λ + Λ ¯ $$ \overline{\Lambda} ...

    S. Acharya, D. Adamová, A. Adler, J. Adolfsson in Journal of High Energy Physics (2020)

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