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      Suppression of contributions from large-parton-number Fok states to T-odd distribution functions in Drell-Yan scattering involving small-x annihilating quark and antiquark

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          Abstract

          T-odd distributions like Sivers and Boer-Mulders functions are normally modeled using few-body models. In the present work I want to follow the completely opposite point of view, and study a high-energy proton-proton Drell-Yan where both the annihilating partons are wee, and one (at least) comes from a high-order Fok state of the parent proton, i.e. a state where a large number N of partons is present. I show that rescattering between active and spectator partons is modified, with suppression of those terms that are needed to build T-odd parton distributions.

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          Single transverse spin asymmetries

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            Transverse-momentum distributions in a diquark spectator model

            All the leading-twist parton distribution functions are calculated in a spectator model of the nucleon, using scalar and axial-vector diquarks. Single gluon rescattering is used to generate T-odd distribution functions. Different choices for the diquark polarization states are considered, as well as a few options for the form factor at the nucleon-quark-diquark vertex. The results are listed in analytic form and interpreted in terms of light-cone wave functions. The model parameters are fixed by reproducing the phenomenological parametrization of unpolarized and helicity parton distributions at the lowest available scale. Predictions for the other parton densities are given and, whenever possible, compared with available phenomenological parametrizations.
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              A Unified Picture for Single Transverse-Spin Asymmetries in Hard Processes

              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, \(q_\perp \gg \Lambda_{\rm QCD}\), and time-reversal-odd and transverse-momentum-dependent parton distributions when \(q_\perp\) 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.
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                Author and article information

                Journal
                23 March 2010
                Article
                1003.4506
                3f7504d3-70c6-49ec-8519-a1e415372671

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                12 pages, 2 figures
                hep-ph

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