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arXiv 2406.00271hep-ph
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在EIC上通过J/ψ和π介子产生揭示胶子TMDs

Unraveling Gluon TMDs in $J/ψ$ and Pion production at the EIC

Khatiza Banu, Asmita Mukherjee, Amol Pawar, Sangem Rajesh

AI总结:

本文在EIC电子-质子散射的背靠背J/ψ和π±产生过程中,利用NRQCD和TMD因子化框架研究方位角不对称性,证明胶子贡献占主导并给出数值估计。

摘要:

我们研究了电子-质子散射中J/ψ和π±产生的方位角不对称性,例如cos2ϕT和Sivers不对称性,重点关注J/ψ和π介子以几乎背靠背构型产生的情形。电子是非极化的,而质子可以是非极化或横向极化的。对于J/ψ的形成,我们采用非相对论QCD(NRQCD),而π±则通过部分子碎裂产生。在这种运动学条件下,我们利用横向动量依赖因子化框架来计算截面和不对称性。我们同时考虑了夸克和胶子引发的过程,并表明胶子贡献占主导地位。我们提供了方位角不对称性上限的数值估计,并在即将到来的电子-离子对撞机(EIC)可达到的运动学区域内,对胶子横向动量分布(TMDs)采用高斯参数化。

英文摘要:

We investigate the azimuthal asymmetries such as $\cos2{ϕ_T}$ and Sivers symmetry for $J/ψ$ and $π^\pm$ production in electron-proton scattering, focusing on scenarios where the $J/ψ$ and the pion are produced in an almost back-to-back configuration. The electron is unpolarized, while the proton can be unpolarized or transversely polarized. For the $J/ψ$ formation, we use non-relativistic QCD (NRQCD), while $π^\pm$ is formed due to parton fragmentation. In this kinematics, we utilize the transverse momentum-dependent factorization framework to calculate the cross sections and asymmetries. We consider both quark and gluon-initiated processes and show that the gluon contribution dominates. We provide numerical estimates of the upper bounds on the azimuthal asymmetries, as well as employ a Gaussian parametrization for the gluon transverse momentum distributions (TMDs), within the kinematical region accessible by the upcoming Electron-Ion Collider (EIC).

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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