1,085 research outputs found

    A Unified Picture for Single Transverse-Spin Asymmetries in Hard Processes

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    Using Drell-Yan pair production as an example, we explore the relation between two well-known mechanisms for single transverse-spin asymmetries in hard processes: twist-three quark-gluon correlations when the pair's transverse momentum is large, qΛQCDq_\perp \gg \Lambda_{\rm QCD}, and time-reversal-odd and transverse-momentum-dependent parton distributions when qq_\perp is much less than the pair's mass. We find that although the two mechanisms have their own domain of validity, they describe the same physics in the kinematic region where they overlap. This unifies the two mechanisms and imposes an important constraint on phenomenological studies of single spin asymmetries.Comment: 4 pages, 3 figure

    Direct Photons in Nuclear Collisions at FAIR Energies

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    Using the extrapolation of existing data estimations of prompt photon production at FAIR energies have been made. At y=yc.m.y=y_{c.m.} the rapidity density of prompt photons with pt>p_{t}> 1.5 GeV/c per central Au+Au event at 25 AGeV is estimated as 104\sim 10^{-4} . With the planed beam intensity 10910^{9} per second and 1% interaction probability, for 10% of most central events one can expect the prompt photon rate 102\sim 10^{2} photons per second. Direct photons from the hadron scenario of ion collisions generated by the Hadron-String-Dynamics (HSD) transport approach with implemented meson scatterings πρπγ,ππργ\pi\rho\to\pi\gamma, \pi\pi\to\rho\gamma have been analyzed. Photons from short-living resonances (e.g. ωπ0γ\omega \to \pi^{0} \gamma) decaying during the dense phase of the collision should be considered as direct photons. They contribute significantly in the direct photon spectrum at pt=0.51p_{t}=0.5 - 1 GeV/c. At the FAIR energy 25 AGeV in Au+Au central collisions the HSD generator predicts, as a lower estimate, γdirect/γπ0\gamma_{direct}/\gamma_{\pi^{0}} \simeq 0.5% in the region pt=0.51p_{t}=0.5 - 1 GeV/c. At pt=1.52p_{t}=1.5 - 2 GeV/c γprompt/γπ0\gamma_{prompt}/\gamma_{\pi^{0}} \simeq 2%. Thermal direct photons have been evaluated with the Bjorken Hydro-Dynamics (BHD) model. The BHD spectra differ strongly from the HSD predictions. The direct photon spectrum is very sensitive to the initial temperature parameter T0T_{0} of the model. The 10 MeV increase in the T0T_{0} value leads to \sim 2 times higher photon yield.Comment: 9 pages, 5 figures, Talk at the session of Russian Academy of Sciences, ITEP, Moscow, 26 - 30 November 200

    Conatraints on ΔG\Delta G from Prompt Photon plus Jet Production at HERA-N\vec{N}

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    The utility of prompt photon plus associated jet production for constraining the size and shape of the polarized gluon density of the proton ΔG\Delta G is examined at S=40\sqrt{S}=40 GeV, appropriate for the proposed HERA-N\vec{N} polarized pp\vec{p}\vec{p} collider experiment. The calculation is performed at next-to-leading order (O(ααs2\alpha\alpha_s^2)) in QCD. The reliability of the predictions are examined in some detail.Comment: 16 pages, 3 figure

    Polarized semi-inclusive electroweak structure functions at next-to-leading-order

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    We present a next-to-leading order (NLO) computation of the full set of polarized and unpolarized electroweak semi-inclusive DIS (SIDIS) structure functions, whose knowledge is crucial for a precise extraction of polarized parton distributions. We focus on the phenomenology of the polarized structure functions for the kinematical conditions that could be reached in an Electron-Ion-Collider. We show that the NLO corrections are sizeable, particularly in the small-xx range. We test the sensitivity of these structure functions on certain quark distributions and compare it to the situation of inclusive DIS and electromagnetic SIDIS.Comment: 17 pages, 5 figure

    QCD corrections to the longitudinally polarized Drell-Yan process

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    In this paper we calculate the O(αs\alpha_s) corrections to the xFx_F- and yy-distributions of lepton pairs produced in collisions of longitudinally polarized hadrons. The numerical importance of these corrections is studied and consequences for the extraction of the polarized sea quark distributions from a measurement of the longitudinally polarized Drell-Yan cross section are discussed.Comment: 21 pages, LaTeX, 8 figures include

    Effects of the large gluon polarization on xg1d(x)xg_1^d(x) and J/ψ\psi productions at polarized ep and pp collisions

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    The recent SMC data of xg1d(x)xg_1^d(x) are reproduced with the large polarized gluons. To study further the polarized gluon distribution in a proton, we calculate the spin--dependent differential cross section for J/ψ\psi leptoproductions and the two--spin asymmetry for J/ψ\psi hadroproductions. Its experimental implication is discussed.Comment: LaTeX file, 10 pages+6 figures available upon request, KOBE-FHD-93-0
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