Abstract

We investigate the $\mathrm{sin}({\ensuremath{\phi}}_{\mathrm{\ensuremath{\Lambda}}}\ensuremath{-}{\ensuremath{\phi}}_{S})$ single-spin asymmetry in the transversely polarized $\mathrm{\ensuremath{\Lambda}}$ production in semi-inclusive deeply inelastic scattering process within the transverse momentum dependent (TMD) factorization. The asymmetry is contributed by the convolution of the polarizing TMD fragmentation function ${D}_{1T}^{\ensuremath{\perp}}$ of the $\mathrm{\ensuremath{\Lambda}}$ hyperon and the unpolarized TMD distribution function ${f}_{1}$ of the proton target. We adopt the spectator diquark model result and the available parametrization for ${D}_{1T}^{\ensuremath{\perp},{\mathrm{\ensuremath{\Lambda}}}^{\ensuremath{\uparrow}}/q}$ to numerically estimate the $\mathrm{sin}({\ensuremath{\phi}}_{\mathrm{\ensuremath{\Lambda}}}\ensuremath{-}{\ensuremath{\phi}}_{S})$ asymmetry at the kinematical region of the electron ion collider (EIC). To implement the TMD evolution formalism, we apply two different parametrizations on the nonperturbative Sudakov form factors associated with the distribution function of the proton and the fragmentation function of the $\mathrm{\ensuremath{\Lambda}}$. It is found that the two sets of ${D}_{1T}^{\ensuremath{\perp},{\mathrm{\ensuremath{\Lambda}}}^{\ensuremath{\uparrow}}/q}$ lead to different $\mathrm{sin}({\ensuremath{\phi}}_{\mathrm{\ensuremath{\Lambda}}}\ensuremath{-}{\ensuremath{\phi}}_{S})$ asymmetry, particularly in sign. We also discuss the impact of the assumptions and approximations applied in the calculations, which may bring large uncertainties to the results in the EIC. Future measurements on the $\mathrm{sin}({\ensuremath{\phi}}_{\mathrm{\ensuremath{\Lambda}}}\ensuremath{-}{\ensuremath{\phi}}_{S})$ asymmetry with high precision at the EIC can provide important cross checks on the available $\mathrm{\ensuremath{\Lambda}}$ polarizing fragmentation functions, as well as constrain them more stringently.

Highlights

  • Understanding the internal partonic structure of hadrons and the fragmentation mechanism of partons are among the main goals in QCD and high energy physics

  • IV, we present the numerical estimate on the sinðφΛ − φSÞ asymmetry in the e−p → e−Λ↑X process at the kinematical region of the electron ion collider (EIC) with different choices on the nonperturbative part associated with the transverse momentum dependent (TMD) evolution effect

  • The asymmetry arises from the convolution of the polarizing fragmentation function (FF) D⊥1T for Λ hyperon and the unpolarized parton distribution function (PDF) f1 for the proton

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Summary

INTRODUCTION

Understanding the internal partonic structure of hadrons and the fragmentation mechanism of partons are among the main goals in QCD and high energy physics. As an alternative to SIA, the processes eþe− → Λ↑ þ h þ X [17,18,19] and semi-inclusive deep inelastic scattering (SIDIS) lp → l0 þΛ↑ þX have been suggested [17] to study the Λ spin asymmetry, where D⊥1T contribute to the transverse polarization of Λ. After performing all of the approaches above, the important issue is the energy dependence of the TMDs, which is encoded in the TMD evolution equations and will be discussed in detail

THE EVOLUTION OF TMD PDFS AND FFS
Approach I
Approach II
NUMERICAL CALCULATION
CONCLUSION
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