EIC中电子-质子碰撞中线极化胶子分布的探测

R. Kishore, A. Mukherjee
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引用次数: 0

摘要

我们提出了最近在计划中的电子-离子对撞机(EIC)的运动学范围内,在电子-离子对撞机(EIC)的$J/\psi$碰撞中产生的方位不对称性$(cos~2\phi)$的估计[8]。我们发现在EIC可以观察到的小$x$区域有一个小但相当大的不对称。这种不对称性直接探测了Weizsäcker-Williams (WW)型线极化胶子在非极化质子中的分布。在满足$J/\psi$, $z < 1$的能量分数和子过程$\gamma^∗ + g \rightarrow c + \bar{c}+ g$给出领先贡献的运动学区域中,我们计算了次领先阶的不对称性。我们使用彩色单线(CS)模型$J/\psi$生产。我们估计了两个模型的不对称性:(i)高斯型参数化和(ii) McLerran-Venugopalan (MV)模型在小- $x$下的不对称性,并给出了不对称性的上界。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probing linearly polarized gluon distribution in electron-proton collision at EIC
We present a recent estimate [8] of azimuthal asymmetry $(cos~2\phi)$ in $J/\psi$ production in ep collision within the kinematics of the planned electron-ion collider (EIC). We find a small but sizable asymmetry in the small-$x$ region which can be observed at the EIC. This asymmetry directly probes the Weizs\"acker-Williams (WW) type linearly polarized gluon distribution in the unpolarized proton. We calculate the asymmetry at next-to-leading order in the kinematical region which satisfies, energy fraction of $J/\psi$, $z < 1$ and the subprocess $\gamma^∗ + g \rightarrow c + \bar{c}+ g$ gives the leading contribution. We use color singlet (CS) model for $J/\psi$ production. We estimate the asymmetry in two models for TMDs: (i) Gaussian type parameterization and (ii) McLerran-Venugopalan (MV) model at small-$x$ and also we present the upper bound of the asymmetry.
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