309 research outputs found

    Modelling and Measurement of Charge Transfer in Multiple GEM Structures

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    Measurements and numerical simulations on the charge transfer in Gas Electron Multiplier (GEM) foils are presented and their implications for the usage of GEM foils in Time Projection Chambers are discussed. A small test chamber has been constructed and operated with up to three GEM foils. The charge transfer parameters derived from the electrical currents monitored during the irradiation with an Fe-55 source are compared with numerical simulations. The performance in magnetic fields up to 2 T is also investigated.Comment: 21 pages, 16 figures, submitted to NIM-

    The Evidence for a Pentaquark Signal and Kinematic Reflections

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    Several recent experiments have reported evidence for a narrow baryon resonance with positive strangeness (Θ+\Theta^+) at a mass of 1.54 GeV/c2c^2. Baryons with S=+1S=+1 cannot be conventional qqqqqq states and the reports have thus generated much theoretical speculation about the nature of possible S=+1S=+1 baryons, including a 5-quark, or pentaquark, interpretation. We show that narrow enhancements in the K+nK^+n effective mass spectrum can be generated as kinematic reflections resulting from the decay of mesons, such as the f2(1275)f_2(1275), the a2(1320)a_2(1320) and the ρ3(1690)\rho_3(1690).Comment: 4 pages, 4 figure

    Shadowing in the nuclear photoabsorption above the resonance region

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    A model based on the hadronic fluctuations of the real photon is developed to describe the total photonucleon and photonuclear cross sections in the energy region above the nucleon resonances. The hadronic spectral function of the photon is derived including the finite width of vector-meson resonances and the quark-antiquark continuum. The shadowing effect is evaluated considering the effective interaction of the hadronic component with the bound nucleons within a Glauber-Gribov multiple scattering theory. The low energy onset of the shadowing effect is interpreted as a possible signature of a modification of the hadronic spectral function in the nuclear medium. A decrease of the ρ\rho-meson mass in nuclei is suggested for a better explanation of the experimental data.Comment: 8 pages, 7 figure

    Form factors and photoproduction amplitudes

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    We examine the use of phenomenological form factors in tree level amplitudes for meson photoproduction. Two common recipes are shown to be fundamentally incorrect. An alternate form consistent with gauge invariance and crossing symmetry is proposed.Comment: To be published in PR

    A mechanism for the Double-Spin Asymmetry in Electromagnetic ρ\rho Production at HERMES

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    We calculate the contribution of meson and pomeron exchanges to the double-spin asymmetry in ρ\rho-meson electromagnetic production at HERMES energies. We show that the observed double-spin asymmetries, which are large, can be explained by the interference between the natural parity f2f_2-secondary Reggeon and the unnatural parity anomalous f1f_1 exchanges.Comment: 7 pages, 3 figures, Late

    Energy Dependence of the Near-Threshold Total Cross-Section for the pp --> pp eta' Reaction

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    Total cross sections for the pp --> pp eta' reaction have been measured in the excess energy range from Q = 1.53 MeV to Q = 23.64 MeV. The experiment has been performed at the internal installation COSY-11 using a stochastically cooled proton beam of the COoler SYnchrotron COSY and a hydrogen cluster target. The determined energy dependence of the total cross section weakens the hypothesis of the S-wave repulsive interaction between the eta' meson and the proton. New data agree well with predictions based on the phase-space distribution modified by the proton-proton final-state-interaction (FSI) only.Comment: 12 pages, 1 table, 4 figure

    Nucleonic resonance excitations with linearly polarized photon in γpωp\gamma p\to \omega p

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    In this work, an improved quark model approach to the ω\omega meson photo-production with an effective Lagrangian is presented. The {\it t}-channel {\it natural}-parity exchange is taken into account through the Pomeron exchange, while the {\it unnatural}-parity exchange is described by the π0\pi^0 exchange. With a very limited number of parameters, the available experimental data in the low energy regime can be consistently accounted for. We find that the beam polarization observables show sensitivities to some {\it s}-channel individual resonances in the SU(6)O(3)SU(6)\otimes O(3) quark model symmetry limit. Especially, the two resonances P13(1720)P_{13}(1720) and F15(1680)F_{15}(1680), which belong to the representation [56,28,2,2,J][{\bf 56, ^2 8}, 2, 2, J], have dominant contributions over other excited states. Concerning the essential motivation of searching for "missing resonances" in meson photo-production, this approach provides a feasible framework, on which systematic investigations can be done.Comment: 16 pages, Revtex, 9 eps figures, to appear in PR

    Exclusive diffractive processes and the quark substructure of mesons

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    Exclusive diffractive processes on the nucleon are investigated within a model in which the quark-nucleon interaction is mediated by Pomeron exchange and the quark substructure of mesons is described within a framework based on the Dyson-Schwinger equations of QCD. The model quark-nucleon interaction has four parameters which are completely determined by high-energy πN\pi N and KNK N elastic scattering data. The model is then used to predict vector-meson electroproduction observables. The obtained ρ\rho- and ϕ\phi-meson electroproduction cross sections are in excellent agreement with experimental data. The predicted q2q^2 dependence of J/ψJ/\psi-meson electroproduction also agrees with experimental data. It is shown that confined-quark dynamics play a central role in determining the behavior of the diffractive, vector-meson electroproduction cross section. In particular, the onset of the asymptotic 1/q41/q^4 behavior of the cross section is determined by a momentum scale that is set by the current-quark masses of the quark and antiquark inside the vector meson. This is the origin of the striking differences between the q2q^2 dependence of ρ\rho-, ϕ\phi- and J/ψJ/\psi-meson electroproduction cross sections observed in recent experiments.Comment: 53 pages, 23 figures, revtex and epsfig. Minor additions to tex

    Vector Meson Photoproduction with an Effective Lagrangian in the Quark Model

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    A quark model approach to the photoproduction of vector mesons off nucleons is proposed. Its starting point is an effective Lagrangian of the interaction between the vector meson and the quarks inside the baryon, which generates the non-diffractive s- and u- channel resonance contributions. Additional t-channel π0\pi^0 and σ\sigma exchanges are included for the ω\omega and ρ0\rho^0 production respectively to account for the large diffractive behavior in the small tt region as suggested by Friman and Soyeur. The numerical results are presented for the ω\omega and ρ\rho productions in four isospin channels with the same set of parameters, and they are in good agreement with the available data not only in ω\omega and ρ0\rho^0 productions but also in the charged ρ\rho productions where the additional t-channel σ\sigma exchange does not contribute so that it provides an important test to this approach. The investigation is also extended to the ϕ\phi photoproduction, and the initial results show that the non-diffractive behavior of the ϕ\phi productions in the large tt region can be described by the s- and u- channel contributions with significantly smaller coupling constants, which is consistent with the findings in the similar studies in the QHD framework. The numerical investigation has also shown that polarization observables are essential for identifying so-called "missing resonances".Comment: 36 pages, 10 PS figures, extended version of nucl-th/9711061 and nucl-th/9803021, submitted to PR

    Photoproduction of ϱo on hydrogen with tagged photons between 4 and 6 GeV

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    We have measured the reaction γp → pπ+π− in the DESY 1 m Streamer Chamber. The dominant ϱo production is analyzed in terms of various models
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