Abstract

The gluon transversity distribution in the deuteron is defined by the matrix element between linearly-polarized deuteron states, and it could be investigated in proton-deuteron collisions in addition to lepton-deuteron scattering. The linear polarization of photon is often used, whereas it is rarely used for the spin-1 deuteron. Therefore, it is desirable to express deuteron-reaction cross sections in term of conventional deuteron spin polarizations for actual experimental measurements. In this work, we investigate how proton-deuteron Drell-Yan cross sections are expressed by the conventional polarizations for finding the gluon transversity distribution. In particular, we show that the gluon transversity can be measured in the proton-deuteron Drell-Yan process by taking the cross-section difference between the deuteron spin polarizations along the two-transverse axes. Since the gluon transversity does not exist for the spin-1/2 nucleons, a finite gluon transversity of the deuteron could indicate an "exotic" mechanism beyond the simple bound system of the nucleons in the deuteron. Therefore, the gluon transversity is an interesting and appropriate observable to shed light on a new hadronic mechanism in nuclei.

Highlights

  • The gluon transversity distribution in the deuteron is defined by the matrix element between linearly polarized deuteron states, and it could be investigated in proton-deuteron collisions in addition to lepton-deuteron scattering

  • We investigate how proton-deuteron Drell-Yan cross sections are expressed by the conventional polarizations for finding the gluon transversity distribution

  • The nucleon spin used to be explained by a combination of three-quark spins in the nucleon according to the basic quark model

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Summary

INTRODUCTION

The nucleon spin used to be explained by a combination of three-quark spins in the nucleon according to the basic quark model. A hadron with spin more than or equal to 1 is needed for the helicity flip of two units It means that the scaling violation of the quark transversity distributions of the nucleon is much different from the one of the longitudinally polarized ones because they are decoupled from the gluon distribution [13,14]. By finding the azimuthal-angle dependence of the deuteron transverse polarization, the gluon transversity distribution will be measured It is the only experimental project, and such an effort will be continued at Electron-Ion Collider (EIC) [18]. Lepton- and hadron-accelerator measurements are complementary, and both results are essential in establishing hadron structure in a wide kinematical region For such a purpose, we proposed to use the protondeuteron Drell-Yan process with the polarized deuteron for finding the gluon transversity distribution in the deuteron [26].

DEUTERON POLARIZATIONS
Deuteron polarizations and parton correlation functions
Rotations of deuteron polarizations around transverse axes
SUMMARY
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