Fully Unintegrated Parton Correlation Functions and Factorization in Lowest Order Hard Scattering

TL;DR

This paper introduces a new formalism for deeply inelastic lepton-proton scattering using gauge-invariant, universal parton correlation functions that depend on all components of parton momentum, avoiding kinematic approximations.

Contribution

It develops a general, approximation-free factorization formalism based on parton correlation functions, extending the concepts of parton density, fragmentation, and soft factors.

Findings

Defines gauge-invariant, universal parton correlation functions.

Establishes a factorization theorem without kinematic approximations.

Provides a subtraction formalism applicable at leading order.

Abstract

Motivated by the need to correct the potentially large kinematic errors in approximations used in the standard formulation of perturbative QCD, we reformulate deeply inelastic lepton-proton scattering in terms of gauge invariant, universal parton correlation functions which depend on all components of parton four-momentum. Currently, different hard QCD processes are described by very different perturbative formalisms, each relying on its own set of kinematical approximations. In this paper we show how to set up formalism that avoids approximations on final-state momenta, and thus has a very general domain of applicability. The use of exact kinematics introduces a number of significant conceptual shifts already at leading order, and tightly constrains the formalism. We show how to define parton correlation functions that generalize the concepts of parton density, fragmentation function, and soft factor. After setting up a general subtraction formalism, we obtain a factorization theorem. To avoid complications with Ward identities the full derivation is restricted to abelian gauge theories; even so the resulting structure is highly suggestive of a similar treatment for non-abelian gauge theories.