Abstract

We present a calculation of the $cos (2 \phi_h)$ asymmetry in $J/\psi$ production in electron-proton collision at the future electron-ion collider (EIC), a useful channel to probe the gluon TMDs. We calculate the asymmetry at next-to-leading order (NLO) in $\alpha_s$ in the framework of generalized factorization. The dominating sub-process is $\gamma^* +g \rightarrow J/\psi+g$. The production of $J/\psi$ is calculated in the non-relativistic QCD(NRQCD) framework with the inclusion of both color singlet and color octet contributions. Numerical estimates of the $cos(2\phi_h)$ asymmetry are given in the kinematical region to be accessed by the future EIC. The asymmetry depends on the parameterization of the gluon TMDs, as well as on the long distance matrix elements (LDMEs). We use both Gaussian-type parameterization and McLerran-Venugopalan model for the TMDs in the kinematical region of small-$x$, where the gluons play a dominant role. We obtain sizable asymmetry, which may be useful to probe the ratio of the linearly polarized and the unpolarized gluon distribution in the proton.

Highlights

  • Quantum chromodynamics (QCD) is an exceptionally rich and complex theory of strong interactions between quarks and gluons, the fundamental constituents of matter

  • The hadron physics community has expanded its inquiry beyond the ordinary one-dimensional collinear parton distribution functions (PDFs) in the motion of the parton and its spatial distribution in a direction perpendicular to the momentum of the parent hadron

  • To account for transverse motion, the collinear PDFs were extended to transverse-momentum-dependent PDFs, referred to as transverse momentum dependent parton distributions (TMDs)[1–3]

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Summary

Introduction

Quantum chromodynamics (QCD) is an exceptionally rich and complex theory of strong interactions between quarks and gluons, the fundamental constituents of matter. These quarks and gluons do not exist in nature as free particles but are confined inside hadrons, and their fundamental properties can be explored only with the help of scattering processes. To account for transverse motion, the collinear PDFs were extended to transverse-momentum-dependent PDFs, referred to as transverse momentum dependent parton distributions (TMDs)[1–3]. TMDs are considered as an extension of the standard, one-dimensional PDFs to the three-dimensional momentum space. Unlike collinear PDFs, which are universal, TMDs are process dependent due to their

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