Abstract

In this paper, we study the single spin asymmetry ${A}_{UT}^{\mathrm{sin}({\ensuremath{\phi}}_{h}\ensuremath{-}{\ensuremath{\phi}}_{S})}$ of a single hadron production in semi-inclusive deep inelastic scattering within the framework of transverse momentum dependent factorization up to the next-to-leading logarithmic order of QCD. The asymmetry is a contribution of the convolution of the Sivers function and the unpolarized fragmentation function. Specifically, the Sivers function in the coordinate space and perturbative region can represent the convolution of the $C$ coefficients and the corresponding collinear correlation functions, among which the Qiu-Sterman function is the most relevant one. We perform a detailed phenomenological analysis of the Sivers asymmetry at the kinematics of the HERMES and the COMPASS measurements. It is found that the obtained ${x}_{B}$-, ${z}_{h}$-, and ${P}_{h\ensuremath{\perp}}$-dependent asymmetries are basically consistent with the HERMES and the COMPASS measurements.

Highlights

  • Since they were first observed, transverse single spin asymmetries (SSA) are a topic in spin physics of significant theoretical and experimental interest [1,2,3]

  • II, we review the basic framework of transverse momentum dependent (TMD) evolution for accessing the Sivers asymmetry in the semiinclusive deep inelastic scattering (SIDIS) process

  • We study the single spin asymmetry AUsinTðφh−φSÞ of a single hadron production in SIDIS within the framework of TMD factorization up to next-to-leading logarithmic (NLL) order of QCD

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Summary

INTRODUCTION

Since they were first observed, transverse single spin asymmetries (SSA) are a topic in spin physics of significant theoretical and experimental interest [1,2,3]. The first one is the transverse momentum dependent (TMD) factorization approach [4,5], where the inclusive cross section is written as a convolution of transverse momentum dependent partonic distribution functions (TMD-PDFs), transverse momentum dependent fragmentation functions (TMDFFs), and QCD partonic cross sections This method is phenomenologically well studied in Refs. We perform the TMD evolution to reach the fragmentation function and Qiu-Sterman function at an initial scale μb 1⁄4 c=bà by the evolution package QCDNUM [32].

FRAMEWORK
F UU and FαUT can be written as
The unpolarized differential cross section
The Sivers differential cross section
NUMERICAL CALCULATION
CONCLUSION
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