Abstract

We evaluate the light-cone operator product expansion for unpolarized transverse momentum dependent (TMD) operator in the background-field technique up twist-3 inclusively. The next-to-leading order (NLO) matching coefficient for the Sivers function is derived. The method, as well as many details of the calculation are presented.

Highlights

  • The exploration of the internal structure of nuclei is a fascinating task, which identifies transverse momentum dependent (TMD) distributions as one of its most powerful tools

  • We evaluate the light-cone operator product expansion for unpolarized transverse momentum dependent (TMD) operator in the background-field technique up twist-3 inclusively

  • Within the TMD factorization approach, the information on hadron structure is encoded in TMD parton distribution functions (TMDPDFs) and TMD fragmentation functions (TMDFFs)

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Summary

Introduction

The exploration of the internal structure of nuclei is a fascinating task, which identifies transverse momentum dependent (TMD) distributions as one of its most powerful tools. We articulate the role of the gauge links and their direction and show (at the level of operators) the famous sing-change in-between DY and SIDIS definitions of the Sivers function [50] Motivated by these considerations, we provide a detailed and pedagogical explanation of the calculation method, which is a major target of this article. The discussion and comparison with earlier calculations is given in 7.3

Sivers effect and TMD factorization
Sivers function in DY
TMD evolution and operator product power expansion
Definition of TMD distributions
Evolution and renormalization
Light-cone OPE at leading order
Light-cone OPE in the light-cone gauge
Light-cone OPE for the gluon TMD operator
Light-cone OPE at next-to-leading order
OPE in background field method
QCD in background field
Evaluation of diagrams
Treatment of rapidity divergences
Renomalization
Difference in the evaluation of DY and SIDIS operators
Definition of collinear distributions
Quark distributions
Gluon distributions The gluon operators of twist-2 and twist-3 are
Small-b expansion for unpolarized and Sivers distributions
From operators to distributions and tree level results
Results at NLO
Discussion and comparison with earlier calculations
Conclusion
A Parametrization of twist-3 operators and decomposition of 3-tensors
B Example of evaluation: diagram E
Evaluation of contribution to OPE The diagram reads
Evaluation of matrix element
C Diagram-by-diagram expressions
Full Text
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