Abstract

We perform a global fit of the available polarized Semi-Inclusive Deep Inelastic Scattering (SIDIS), polarized pion-induced Drell-Yan (DY) and W±/Z boson production data at N3LO and NNLO accuracy of the Transverse Momentum Dependent (TMD) evolution, and extract the Sivers function for u, d, s and for sea quarks. The Qiu-Sterman function is determined in a model independent way via the operator product expansion from the extracted Sivers function. The analysis is supplemented by additional studies, such as the estimation of applicability region, the impact of the unpolarized distributions’ uncertainties, the universality of the Sivers functions, positivity constraints, the significance of the sign-change relation, and the comparison with the existing extractions.

Highlights

  • Data with next-to-next-to-leading order (NNLO) and next-to-next-to-next-to-leading order (N3LO) of Transverse Momentum Dependent (TMD) evolution and provide a detailed description of results presented in ref. [10]

  • Ref. [10], we demonstrate the universality of the Sivers function and describe simultaneously Semi-Inclusive Deep Inelastic Scattering (SIDIS), Drell-Yan, and W ±/Z boson production data using TMD evolution and the universal nonperturbative CS kernel extracted from the unpolarized measurements

  • We describe in detail results of N3LO extraction of the Sivers function, presented in ref

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Summary

Formalism

We start by summarizing theoretical formalism and presenting expressions that describe DY process and SIDIS cross-sections within TMD factorization. Find details about TMD factorization and derivations of cross-sections for these processes in refs. [4, 13, 15, 23, 68, 71]

Definition of TMD distributions
Sivers asymmetry in SIDIS
Transverse single-spin asymmetry in DY process
Nonperturbative parametrization for the Sivers function
Data selection
Fit procedure and estimation of uncertainties
Test of the factorization region limit
Results of extraction
Fit of the data
Sivers function in the position and the momentum spaces
Positivity constraints for the Sivers function
Determination of the Qiu-Sterman function
Analysis of the sign change
Conclusions
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