Elastic scattering of a quark from a color field: longitudinal momentum exchange
arXiv:1708.07533 · doi:10.1103/PhysRevD.96.074020
Abstract
Perturbative QCD in the small Bjorken limit can be formulated as an effective theory known as the Color Glass Condensate (CGC) formalism. The CGC formalism takes into account the dynamics of large gluon densities at small and has been successfully applied to Deep Inelastic Scattering (DIS) and particle production in high energy hadronic and nuclear collisions in the small kinematic region. The effective degrees of of freedom in CGC are Wilson lines which enter in the effective quark (and gluon) propagators and re-sum multiple soft scatterings from the small gluon field of the target. It is however known that the CGC effective theory breaks down when one probes the moderately large (high ) kinematics where collinear factorization and DGLAP evolution of parton distribution functions should be the right framework. Here we propose a general framework which may allow one to eventually unify the two approaches and to calculate pQCD cross sections in both small and large Bjorken regions. We take the first step towards this goal by deriving an expression for the quark propagator in a background field which includes scatterings from both small and large modes of the gluon field of the target. We describe how this quark propagator can be used to calculate QCD structure functions and at all and thus generalize the dipole model of DIS. We outline this approach can also be used to extend the so-called hybrid approach to particle production in the forward rapidity region of high energy hadronic and nuclear collisions to all and regions and speculate on how one may apply the same techniques to extend the McLerran-Venugopalan effective action used in high energy heavy ion collisions to include high physics.
arXiv comment22 pages, 14 figures
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