236 research outputs found

    Hard Pomeron in exclusive meson production at ILC

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    We calculate the exclusive process gamma* gamma* ->rho rho at high energy. The Born order estimate and the leading (LLA) and next to leading order (NLLA) BFKL resummation effects show the feasibility of experimental detection in a quite large range of Q2 values at future high energy e+e- linear colliders.Comment: 4 pages, Presented at Photon2005, International Conference on the Structure and Interactions of the Photon, Warsaw 31.08-04.09.2005, by Samuel Wallo

    Probing Transversity GPDs in Photo and Electroproduction of Two Vector Mesons

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    Electroproduction of two mesons well separated in rapidity allows the first feasible selective access to chiral-odd transversity GPDs provided one of these mesons is a transversely polarized vector meson rho_T.Comment: 3 pages, 5 figures, to be published in the proceedings of the International Conference on the Structure and Interactions of the Photon (Photon 2007) Paris, july 200

    Testing the dynamics of high energy scattering using vector meson production

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    I review work on diffractive vector meson production in photon-proton collisions at high energy and large momentum transfer, accompanied by proton dissociation and a large rapidity gap. This process provides a test of the high energy scattering dynamics, but is also sensitive to the details of the treatment of the vector meson vertex. The emphasis is on the description of the process by a solution of the non-forward BFKL equation, i.e. the equation describing the evolution of scattering amplitudes in the high-energy limit of QCD. The formation of the vector meson and the non-perturbative modeling needed is also briefly discussed.Comment: 17 pages, 8 figures. Brief review to appear in Mod. Phys. Lett.

    Transversity GPD in photo- and electroproduction of two vector mesons

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    The chiral-odd generalized parton distribution (GPD), or transversity GPD, of the nucleon can be accessed experimentally through the photo- or electroproduction of two vector mesons on a polarized nucleon target, \gamma^(*) N --> \rho_1 \rho_2 N', where \rho_1 is produced at large transverse momentum, \rho_2 is transversely polarized, and the mesons are separated by a large rapidity gap. We predict the cross section for this process for both transverse and longitudinal \rho_{2} production. To this end we propose a model for the transversity GPD H_T(x,\xi,t), and give an estimate of the relative sizes of the transverse and longitudinal \rho_{2} cross sections. We show that a dedicated experiment at high energy should be able to measure the transversity content of the proton.Comment: 15 pages, 9 figures. Extended discussion of experimental prospects in the conclusions. Version to appear in EPJ

    Hard exclusive reactions and hadron structure

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    The generalized Bjorken regime of exclusive reactions opens new ways to explore the hadron structure. We shortly review the present status of this domain where generalized parton distributions, generalized distribution amplitudes and transition distribution amplitudes describe various aspects of confinement physics.Comment: 7 pages LATEX, 5 figures, invited talk at the Vth Conference on Hadronic Physics held at ICTP, Trieste, Italy, May 200

    Vector Meson Photoproduction from the BFKL Equation II: Phenomenology

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    Diffractive vector meson photoproduction accompanied by proton dissociation is studied for large momentum transfer. The process is described by the non-forward BFKL equation which we use to compare to data collected at the HERA collider.Comment: 39 pages, 29 figure

    DGLAP versus perturbative Pomeron in large momentum transfer hard diffractive processes at HERA and LHC

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    We evaluate within the LO DGLAP approximation the dependence on energy of the cross section of the photo(electro)production of vector meson V (V=J/ψ,...V=J/\psi,...) in the hard elastic processes off a parton γ∗+g→V=J/ψ+g\gamma^*+g\to V=J/\psi+g as the function of momentum transfer t=(qγ−pV)2t=(q_{\gamma}-p_V)^2. We demonstrate that in the limit −t≄mV2+Q2-t \ge m_V^2 +Q^2 the cross section does not contain double logarithmic terms in any order of the DGLAP approximation leading to the energy independent cross section. Thus the energy dependence of cross section γ∗+p→J/ψ+rapidity gap+X\gamma^*+p\to J/\psi+{\rm rapidity ~gap} +X is governed at large tt by the gluon distribution within a proton, i.e. it is unambiguously predicted within the DGLAP approximation including the stronger WÎłNW_{\gamma N} dependence at larger −t-t . This prediction explains recent HERA data. The calculations which follow perturbative Pomeron logic predict opposite trend of a weaker WÎłNW_{\gamma N} dependence at larger tt. We explain that at the HERA energies double logarithmic terms characteristic for DGLAP approximation dominate in the hard processes as the consequence of constraints due to energy-momentum conservation. We give predictions for ultraperipheral hard diffractive processes at the LHC and show that these processes are well suited for looking for the contribution of the single logarithmic terms due to the gluon emission in the multiRegge kinematics. We also comment on the interrelation between energy and tt dependence of the cross sections of the hard exclusive processes.Comment: 12 pages, 3 figure

    Gaps between Jets in the High Energy Limit

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    We use perturbative QCD to calculate the parton level cross section for the production of two jets that are far apart in rapidity, subject to a limitation on the total transverse momentum Q0 in the interjet region. We specifically address the question of how to combine the approach which sums all leading logarithms in Q/Q0 (where Q is the jet transverse momentum) with the BFKL approach, in which leading logarithms of the scattering energy are summed. This paper constitutes progress towards the simultaneous summation of all important logarithms. Using an "all orders" matching, we are able to obtain results for the cross section which correctly reproduce the two approaches in the appropriate limits.Comment: 29 pages, 9 figures, minor corrections to text and improved figure

    Rapidity gaps at HERA and the Tevatron from soft colour exchanges

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    Models based on soft colour exchanges to rearrange colour strings in the final state provide a general framework for both diffractive and non-diffractive events in ep and hadron-hadron collisions. We study two such models and find that they can reproduce rapidity gap data from both HERA and the Tevatron. We also discuss the influence of parton cascades and multiple interactions on the results.Comment: 4 pages, 4 EPS figures, presented at UK Phenomenology Workshop on Collider Physics, Durham. Uses iopart.cl

    QCD factorizations in gamma* gamma* -> rho rho

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    We calculate the lowest order QCD amplitude, i.e. the quark exchange contribution, to the forward production amplitude of a pair of longitudinally polarized ρ\rho mesons in the scattering of two virtual photons γ∗(Q1)γ∗(Q2)→ρL0ρL0\gamma^*(Q_1) \gamma^*(Q_2) \to \rho^0_L \rho^0_L. We show that the scattering amplitude simultaneously factorizes in two quite different ways: the part with transverse photons is described by the QCD factorization formula involving the generalized distribution amplitude of two final ρ\rho mesons, whereas the part with longitudinally polarized photons takes the QCD factorized form with the ÎłL∗→ρL0\gamma^*_L \to \rho^0_L transition distribution amplitude. Perturbative expressions for these, in general, non-perturbative functions are obtained in terms of the ρ−\rho-meson distribution amplitude
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