Abstract

We show possible transverse-momentum-dependent parton distribution functions (TMDs) for spin-1 hadrons including twist-3 and 4 functions in addition to the leading twist-2 ones by investigating all the possible decomposition of a quark correlation function in the Lorentz-invariant way. The Hermiticity and parity invariance are imposed in the decomposition; however, the time-reversal invariance is not used due to an active role of gauge links in the TMDs. Therefore, there exist time-reversal-odd functions in addition to the time-reversal even ones in the TMDs. We list all the functions up to twist-4 level because there were missing terms associated with the lightcone vector $n$ in previous works on the twist-2 part and there was no correlation-function study in the twist-3 and 4 parts for spin-1 hadrons. We show that 40 TMDs exist in the tensor-polarized spin-1 hadron in twists 2, 3, and 4. Some expressions of twist-2 structure functions are modified from previous derivations due to the new terms with $n$, and we find 30 new structure functions in twists 3 and 4 in this work. Since time-reversal-odd terms of the collinear correlation function should vanish after integrals over the partonic transverse momentum, we obtain new sum rules for the time-reversal-odd structure functions, $ \int d^2 k_T h_{LT}= \int d^2 k_T h_{LL} = \int d^2 k_T h_{3LL} =0$. In addition, we indicate that new transverse-momentum-dependent fragmentation functions exist in tensor-polarized spin-1 hadrons. The TMDs are rare observables to find explicit color degrees of freedom in terms of color flow, which cannot be usually measured because the color is confined in hadrons.

Highlights

  • It had been taken for granted that the proton spin consists of three quark spins in the naive quark model

  • In order to figure out the partonic OAM contributions, one needs to study three-dimensional (3D) structure functions which include generalized parton distributions (GPDs) [3], generalized distribution amplitudes (GDAs or timelike GPDs) [4], and transverse-momentumdependent parton distributions (TMDs) [5]

  • The path dependence of the gauge link is important in TMD physics, as we show the difference between the TMDs of the semi-inclusive deep inelastic scattering (SIDIS) and the Drell-Yan process in the following

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Summary

Introduction

It had been taken for granted that the proton spin consists of three quark spins in the naive quark model. The color flow appears explicitly in the TMDs, it does not show up in other observables because of the color confinement. They have interesting application to other fields of physics, such as the gluon condensate [6], color

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