Leading twist nuclear shadowing, nuclear generalized parton distributions and nuclear DVCS at small x

TL;DR

This paper extends the leading twist theory to calculate nuclear generalized parton distributions, predicting significant nuclear shadowing effects and their impact on DVCS observables at small x, especially for heavy nuclei like Pb-208.

Contribution

It provides the first detailed calculation of nuclear GPDs incorporating shadowing effects and predicts observable consequences for DVCS and beam-spin asymmetries at high energies.

Findings

Nuclear shadowing causes large suppression of nuclear GPDs.

DVCS cross section is dominated by nuclear effects at high energies.

Nuclear shadowing induces oscillations in the beam-spin asymmetry A_{LU}.

Abstract

We generalize the leading twist theory of nuclear shadowing and calculate quark and gluon generalized parton distributions (GPDs) of spinless nuclei. We predict very large nuclear shadowing for nuclear GPDs. In the limit of the purely transverse momentum transfer, our nuclear GPDs become impact-parameter-dependent nuclear parton distributions (PDFs). Nuclear shadowing induces nontrivial correlations between the impact parameter b and the light-cone fraction x. We make predictions for the deeply virtual Compton scattering (DVCS) amplitude and the DVCS cross section on Pb-208 at high energies. We calculate the cross section of the Bethe-Heitler (BH) process and address the issue of the extraction of the DVCS signal from the e A \to e \gamma A cross section. We find that the e A \to e \gamma A differential cross section is dominated by DVCS at the momentum transfer t near the minima of the nuclear form factor. We also find that nuclear shadowing leads to dramatic oscillations of the DVCS beam-spin asymmetry, A_{LU}, as a function of t. The position of the points where A_{LU} changes sign is directly related to the magnitude of nuclear shadowing.