Abstract

The dual parametrization and the Mellin-Barnes integral approach represent two frameworks for handling the double partial wave expansion of generalized parton distributions (GPDs) in the conformal partial waves and in the $t$-channel ${\rm SO}(3)$ partial waves. Within the dual parametrization framework, GPDs are represented as integral convolutions of forward-like functions whose Mellin moments generate the conformal moments of GPDs. The Mellin-Barnes integral approach is based on the analytic continuation of the GPD conformal moments to the complex values of the conformal spin. GPDs are then represented as the Mellin-Barnes-type integrals in the complex conformal spin plane. In this paper we explicitly show the equivalence of these two independently developed GPD representations. Furthermore, we clarify the notions of the $J=0$ fixed pole and the $D$-form factor. We also provide some insight into GPD modeling and map the phenomenologically successful Kumeri\v{c}ki-M\"uller GPD model to the dual parametrization framework by presenting the set of the corresponding forward-like functions. We also build up the reparametrization procedure allowing to recast the double distribution representation of GPDs in the Mellin-Barnes integral framework and present the explicit formula for mapping double distributions into the space of double partial wave amplitudes with complex conformal spin.

Highlights

  • Meson Production (DVMP)) admitting description within the generalized parton distributions (GPDs) formalism constitute a significant part of the research programs of several existing (JLab, COMPASS) and future (EIC, PANDA @ GSI-FAIR, J-PARC) experimental facilities

  • The conformal partial wave expansion (PWE) of GPDs deals with partial waves (PWs) that are labeled by the complex conformal spin, which characterizes the irreducible multiplets of appropriate conformal operators

  • The problem of building up a phenomenological GPD parametrization capable of describing the whole set of the present day experimental data can be in principle addressed within any GPD representation: double distribution representation, dual parametrization, or MellinBarnes integral representation

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Summary

Notations and conventions

The conformal partial wave expansion (PWE) of GPDs deals with partial waves (PWs) that are labeled by the complex conformal spin, which characterizes the irreducible multiplets of appropriate conformal operators. Both quark and antiquark GPDs are even in skewness η and satisfy the polynomiality constraints. It is convenient to introduce the conformal PWs pn(x, η) including both the integration weight and the support restrictions, expressed by the θ-function, pn(x, η) = η−n−1pn(x/η) , pn(x) θ(1. For integer values of the conformal spin the conformal PWE of a generic quark GPD F q is formally given by. Spoken one might view the integral conformal PWE (2.11) as a GPD representation in the space of singular generalized functions. This series requires rigorous definition in the mathematical sense.

Summing up conformal partial waves with the Mellin-Barnes techniques
Dual parametrization
Basics of the dual parametrization
Special limiting cases
Elementary amplitude
Calculation of the D-form factor
GPD model examples
A generic model for the dual parametrization
KM10 model
Partial wave amplitudes from double distributions
Conclusions
Full Text
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