Abstract

In this work, we present a new set of unpolarized ($ H $) and polarized ($\widetilde{H}$) generalized parton distributions (GPDs) that have been determined using a simultaneous $ \chi^2 $ analysis of the nucleon axial form factor (AFF) and wide-angle Compton scattering (WACS) experimental data at the next-to-leading order (NLO) accuracy in QCD. We explore various Ansatzes presented in the literature for GPDs, which use forward parton distributions as input, and choose the ones most suited to our analysis. The experimental data included in our analysis cover a wide range of the squared transverse momentum, which is $ 0.025 < -t < 6.46 $ GeV$ ^2 $. We show that the WACS data affect significantly the large $-t$ behavior of $\widetilde{H}$. The polarized GPDs obtained from the simultaneous analysis of AFF and WACS data differ considerably from the corresponding ones obtained by analyzing AFF and WACS separately, and have less uncertainties. We show that the theoretical predictions obtained using our GPDs are in good agreement with the analyzed AFF and WACS data for the entire range of $ -t $ studied. Finally, we obtain the impact parameter dependent parton distributions, both in an unpolarized and in a transversely polarized proton, and present them as tomography plots.

Highlights

  • The factorization theorem has been very successful in describing perturbative quantum chromodynamics (QCD) processes, considering them as being composed of a soft nonperturbative and a hard parton level part

  • We have performed various analyses using different sets of parton distribution functions (PDFs) to study the sensitivity of the fit results to the PDFs set that we choose for calculating the generalized parton distributions (GPDs) H and the resulting wide-angle Compton scattering (WACS) cross section

  • We have shown that there are no significant differences between the analyses performed using different sets of PDFs in view of χ2 and parameter values, the extracted GPDs differ as functions of x, especially for the case of down valence and sea quark distributions

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Summary

Introduction

The factorization theorem has been very successful in describing perturbative quantum chromodynamics (QCD) processes, considering them as being composed of a soft nonperturbative and a hard parton level (perturbatively calculable) part. It is well known that the nonperturbative part can be described using the language of parton distribution functions (PDFs) [1,2,3,4,5,6,7,8,9,10,11] and polarized PDFs (PPDFs) [12,13,14,15,16,17,18,19,20,21,22]

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