1,079 research outputs found

    Studies of spin-orbit correlations at JLAB

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    Studies of single spin asymmetries for pion electroproduction in semi-inclusive deep-inelastic scattering are presented using the polarized \sim6 GeV electrons from at the Thomas Jefferson National Accelerator Facility (JLab) and the Continuous Electron Beam Accelerator Facility (CEBAF) Large Acceptance Spectrometer (CLAS) with the Inner Calorimeter. The cross section versus the azimuthal angle {\phi}_h of the produced neutral pion has a substantial sin {\phi}_h amplitude. The dependence of this amplitude on Bjorken x_B and on the pion transverse momentum is extracted and compared with published data.Comment: proceedings of SPIN2010 conference (September-October 2010, Juelich-Germany

    Monte Carlo simulation of single spin asymmetries in pion-proton collisions

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    We present Monte Carlo simulations of both the Sivers and the Boer-Mulders effects in the polarized Drell-Yan π±pμ+μX\pi^\pm p^\uparrow \to \mu^+ \mu^- X process at the center-of-mass energy s14\sqrt{s} \sim 14 GeV reachable at COMPASS with pion beams of energy 100 GeV. For the Sivers effect, we adopt two different parametrizations for the Sivers function to explore the statistical accuracy required to extract unambiguous information on this parton density. In particular, we verify the possibility of checking its predicted sign change between Semi-Inclusive Deep-Inelastic Scattering (SIDIS) and Drell-Yan processes, a crucial test of nonperturbative QCD. For the Boer-Mulders effect, because of the lack of parametrizations we can make only guesses. The goal is to explore the possibility of extracting information on the transversity distribution, the missing piece necessary to complete the knowledge of the nucleon spin structure at leading twist, and the Boer-Mulders function, which is related to the long-standing problem of the violation of the Lam-Tung sum rule in the unpolarized Drell-Yan cross section.Comment: RevTeX, 13 pages, 7 figures included in .eps forma

    Quark orbital angular momentum: can we learn about it from GPDs and TMDs?

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    It is known how to access information on quark orbital angular momentum from generalized parton distribution functions, in a certain specified framework. It is intuitively expected, that such information can be accessed also through transverse momentum dependent distribution functions, but not known how. Now quark models provide promising hints. Recent results are reviewed.Comment: proceeding of the "4th Workshop on Exclusive Reactions at High Momentum Transfer," 18-21 May 2010, Jefferson La

    Predictions for double spin asymmetry A_{LT} in Semi Inclusive DIS

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    In the leading order of QCD parton model of Semi Inclusive Deep Inelastic Scattering (SIDIS) the double spin asymmetry ALTA_{LT} arises due to the longitudinal polarization of quarks in the transversely polarized nucleon. The corresponding kT2k_T^2 weighted distribution function g1T(1)g^{(1)}_{1T} can be related to ordinary helicity distribution g1(x)g_1(x) measured in DIS. Using recent parameterizations for (un)polarized distribution and fragmentation functions we calculated ALTA_{LT} asymmetry on transversely polarized proton and deuteron targets for different types hadron production. The predictions are given for COMPASS, HERMES and JLab energies. The role of Lorentz invariance relations and positivity constraints are discussed.Comment: The new conventional definition of asymmetry is adopted -- the factor two is added. The figures are rescaled by factor tw

    Performance of the Electromagnetic Calorimeter of the HERMES Experiment

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    The performance of the electromagnetic calorimeter of the HERMES experiment is described. The calorimeter consists of 840 radiation resistant F101 lead-glass counters. The response to positrons up to 27.5 GeV, the comparison between the measured energy and the momentum reconstructed from tracking, long-term stability, hadron rejection and neutral meson invariant mass reconstruction are shown.Comment: 22 pages, 13 figures, LaTeX, accepted by NI
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