Quark-antiquark asymmetry of helicity distributions in the nucleon sea

被引:4
|
作者
Liu, Mengyun [1 ,2 ]
Ma, Bo-Qiang [1 ,2 ,3 ,4 ]
机构
[1] Peking Univ, Sch Phys, Beijing 100871, Peoples R China
[2] Peking Univ, State Key Lab Nucl Phys & Technol, Beijing 100871, Peoples R China
[3] Collaborat Innovat Ctr Quantum Matter, Beijing, Peoples R China
[4] Peking Univ, Ctr High Energy Phys, Beijing 100871, Peoples R China
基金
中国国家自然科学基金;
关键词
DEEP-INELASTIC-SCATTERING; SPIN STRUCTURE-FUNCTION; STRUCTURE-FUNCTION G(1)(P); STRUCTURE-FUNCTION G1(X); STRANGE-ANTISTRANGE SEA; N-C LIMIT; FLAVOR-ASYMMETRY; PARTON DISTRIBUTIONS; SYMMETRY-BREAKING; WAVE-FUNCTION;
D O I
10.1103/PhysRevD.98.036024
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study the helicity distributions of light flavor quark-antiquark (q (q) over bar) 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 (q) over bar pairs are treated from statistical consideration by introducing the helicity suppression factors l(q)(x) and (l) over bar (q)(x) to parametrize the helicity distributions of q-flavor sea quark and antiquark respectively, while Delta l(q)(x) = l(q)(x) - (l) over bar (q)(x) represents a combined effect of helicity contribution due to sea q (q) over bar pairs. From fitting the nucleon polarization asymmetries A(1)(N) in inclusive deep inelastic scattering processes and the single-spin asymmetries A(L)(W +/-) 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 q (q) over bar pairs, i.e., Delta q(s)(x) not equal Delta(q) over bar (s)(x), plays an important role for a comprehensive understanding of the nucleon spin content.
引用
收藏
页数:10
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