Abstract

Experimental processes that are sensitive to parton Wigner distributions provide a powerful tool to advance our understanding of proton structure. In this work, we compute gluon Wigner and Husimi distributions of protons within the Color Glass Condensate framework, which includes a spatially dependent McLerran-Venugopalan initial configuration and the explicit numerical solution of the JIMWLK equations. We determine the leading anisotropy of the Wigner and Husimi distributions as a function of the angle between impact parameter and transverse momentum. We study experimental signatures of these angular correlations at a proposed Electron Ion Collider by computing coherent diffractive dijet production cross sections in e+p collisions within the same framework. Specifically, we predict the elliptic modulation of the cross section as a function of the relative angle between nucleon recoil and dijet transverse momentum for a wide kinematical range. We further predict its dependence on collision energy, which is dominated by the growth of the proton with decreasing $x$.

Highlights

  • Diffractive processes in deep inelastic scattering of electrons off protons or heavier nuclei can provide important information on the target’s structure in coordinate and momentum space [1]

  • We focus on dijet kinematics in the so-called correlation limit and predict the dependence of elliptic modulations as a function of the relative angle between the nucleon recoil and dijet transverse momentum on collision energy and kinematics, which can be tested at a future electron-ion collider (EIC)

  • IV we present our results for diffractive dijet production cross sections in e þ p collisions at typical EIC energies

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Summary

INTRODUCTION

Diffractive processes in deep inelastic scattering of electrons off protons or heavier nuclei can provide important information on the target’s structure in coordinate and momentum space [1]. At very small x the color glass condensate effective theory, describing quantum chromodynamics (QCD) in the high-energy limit, is a suitable framework to compute diffractive processes In this framework, slow modes in the fast-moving target are highly occupied gluon fields, which can be described classically by the Yang-Mills equations. We focus on dijet kinematics in the so-called correlation limit and predict the dependence of elliptic modulations as a function of the relative angle between the nucleon recoil and dijet transverse momentum on collision energy and kinematics, which can be tested at a future EIC We compute diffractive cross sections for charm jets from the CGC in Sec. IV B and study the dependence of the elliptic Fourier coefficient on the dijet momentum, photon virtuality and collision energy. In Appendix B we discuss conventions for transverse dijet momentum variables and in Appendix C we investigate the dependence of azimuthal dijet correlations on the proton size

The structure of nucleons from Wigner distributions
Nc tr b þ r 2
Diffractive dijet production in the dipole picture
The dipole amplitude at small xP
IP-Sat model
Color glass condensate computation
COHERENT DIFFRACTIVE DIJET PRODUCTION
Baseline study
CGC computation
Findings
CONCLUSIONS
Full Text
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