Abstract

We study the helicity distributions of light flavor quark-antiquark ($q \bar{q}$) pairs in the nucleon sea. The valence quarks are handled by adopting the light-cone SU(6) quark-spectator-diquark model and the sea $q \bar{q}$ pairs are treated from statistical consideration by introducing the helicity suppression factors $l_q(x)$ and $\bar l_q(x)$ to parametrize the helicity distributions of q-flavor sea quark and antiquark respectively, while $\Delta l_q(x)=l_q(x)-\bar l_q(x)$ represents a combined effect of helicity contribution due to sea $q \bar{q}$ pairs. From fitting the nucleon polarization asymmetries $A^N_1$ in inclusive deep inelastic scattering processes and the single-spin asymmetries $A^{W^{\pm}}_L$ in Drell-Yan type processes, we find a significant asymmetry between the quark and antiquark helicity distributions of the nucleon sea. Therefore the quark-antiquark asymmetry of helicity distributions of nucleon sea $q \bar{q}$ pairs, i.e., $\Delta q_s(x) \neq \Delta \bar q_s(x)$, plays an important role for a comprehensive understanding of the nucleon spin content.

Highlights

  • The spin structure of hadrons has received considerable attention since the so-called “proton spin crisis” [1,2], which implies that only a small fraction of the proton spin comes from quark spins

  • We investigate the quark-antiquark asymmetry of helicity distributions of the nucleon sea with the valence quarks handled by the light-cone SU(6) quarkspectator-diquark model [10,11,51] and the sea quarks treated by introducing new parameters from statistical consideration

  • The results indicate that the light-cone SU(6) quarkspectator-diquark model, together with the relativistic effect due to quark transversal motions and the quark-antiquark asymmetry of helicity distributions of the nucleon sea with phenomenologically based models and parameters, can provide good descriptions for the physical quantities related to the “proton spin crisis.”

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Summary

INTRODUCTION

The spin structure of hadrons has received considerable attention since the so-called “proton spin crisis” [1,2], which implies that only a small fraction (about 30% in recent studies [3,4,5]) of the proton spin comes from quark spins. The sea quark spin contribution to the proton is believed to be nontrivial, as reflected in the recent observations [21,22] of single spin asymmetries of WÆ production in polarized proton-proton collisions [23,24] It is shown [21] that a reasonable description of WÆ single spin asymmetry data [23] can be achieved by adopting sizable helicity distributions of the light-flavor up (u) and down (d) antiquarks. We investigate the quark-antiquark asymmetry of helicity distributions of the nucleon sea with the valence quarks handled by the light-cone SU(6) quarkspectator-diquark model [10,11,51] and the sea quarks treated by introducing new parameters from statistical consideration.

LIGHT-CONE QUARK-SPECTATORDIQUARK MODEL
NUCLEON POLARIZATION ASYMMETRIES AN1 IN POLARIZED DIS PROCESSES
Findings
SUMMARY
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