932 research outputs found

    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

    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

    Single Transverse-Spin Asymmetry in Drell-Yan Production at Large and Moderate Transverse Momentum

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    We study the single-transverse spin asymmetry for the Drell-Yan process. We consider production of the lepton pair at large transverse momentum, qQq_\perp\sim Q, where QQ is the pair's mass. The spin asymmetry is then of higher twist and may be generated by twist-three quark-gluon correlation functions. Expanding the result for qQq_\perp\ll Q, we make contact with the transverse-momentum-dependent QCD factorization involving the so-called Sivers functions. We find that the two mechanisms, quark-gluon correlations on one hand and the Sivers effect on the other, contain the same physics in this region. This ties the two together and imposes an important constraint on phenomenological studies of single transverse spin asymmetries.Comment: 29 pages, 10 figure

    Drell-Yan forward-backward and spin asymmetries for arbitrary vector boson production at next-to-leading order

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    Longitudinally polarized, unpolarized and forward-backward mass differential cross sections for Drell-Yan lepton-pair production by arbitrary vector bosons are calculated in next-to-leading order (NLO) QCD. Analytical results are presented in a form valid for all consistent nn-dimensional regularization schemes, with the mass factorization scheme kept general. NLO predictions for all Drell-Yan type processes (W±W^\pm, ZZ and γ\gamma^*) at BNL's relativistic heavy ion collider (RHIC) are made using polarized parton distributions which fit the recent deep-inelastic scattering data. These are examined as tools in the determination of the polarized parton distributions and the unpolarized uˉ/dˉ\bar{u}/\bar{d} ratio. NLO predictions for the forward-backward lepton asymmetry at Fermilab are made and the precision determination of sin2θW\sin^2 \theta_W from future runs is studied. In all the above, the QCD corrections are found to be significant. An introductory discussion is given of various theoretical issues, such as allowable factorization and regularization schemes, and scale dependences.Comment: 34 pages, figures included, revtex. Some discussions and references added/modified. In more compact form. To appear in Phys. Rev.

    Next-to-leading order QCD corrections to spin-dependent hadron-pair photoproduction

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    We compute the next-to-leading order QCD corrections to the ``direct'' part of the spin-dependent cross section for hadron-pair photoproduction. The calculation is performed using largely analytical methods. We present a brief phenomenological study of our results focussing on the KK-factors and scale dependence of the next-to-leading order cross sections. This process is relevant for the extraction of the gluon polarization in present and future spin-dependent lepton-nucleon scattering experiments.Comment: 9 pages, 2 eps figure

    Spin Structure Function of the Virtual Photon Beyond the Leading Order in QCD

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    Polarized photon structure can be studied in the future polarized e+ee^{+}e^{-} colliding-beam experiments. We investigate the spin-dependent structure function of the virtual photon g1γ(x,Q2,P2)g_1^{\gamma}(x,Q^2,P^2), in perturbative QCD for Λ2P2Q2\Lambda^2 \ll P^2 \ll Q^2, where Q2-Q^2 (P2-P^2) is the mass squared of the probe (target) photon. The analysis is performed to next-to-leading order in QCD. We particularly emphasize the renormalization scheme independence of the result.The non-leading corrections significantly modify the leading log result, in particular, at large xx as well as at small xx. We also discuss the non-vanishing first moment sum rule of g1γg_1^\gamma, where O(αs){\cal O}(\alpha_s) corrections are computed.Comment: 39 pages, LaTeX, 6 Postscript Figures, eqsection.sty file include

    Next-to-Leading Order Analysis of Inclusive and Semi-inclusive Polarized Data

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    We present a combined next-to-leading order QCD analysis to data on both inclusive and semi-inclusive polarized deep inelastic scattering asymmetries. Performing NLO QCD global fits with different sets of observables, we evaluate the impact of the very recent semi-inclusive results presented by SMC in the extraction of NLO polarized parton distributions.Comment: 22 pages, 4 figures include
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