Perspective on polarised parton distribution functions and proton spin

被引:9
|
作者
Cheng, P. [1 ,2 ]
Yu, Y. [1 ,2 ]
Xing, H. -Y. [1 ,2 ]
Chen, C. [3 ,4 ]
Cui, Z. -F. [1 ,2 ]
Roberts, C. D. [1 ,2 ]
机构
[1] Nanjing Univ, Sch Phys, Nanjing 210093, Jiangsu, Peoples R China
[2] Nanjing Univ, Inst Nonperturbat Phys, Nanjing 210093, Jiangsu, Peoples R China
[3] Univ Sci & Technol China, Interdisciplinary Ctr Theoret Study, Hefei 230026, Anhui, Peoples R China
[4] Peng Huanwu Ctr Fundamental Theory, Hefei 230026, Anhui, Peoples R China
基金
中国国家自然科学基金;
关键词
Proton structure; High-energy polarised proton-proton; collisions; Polarised deep inelastic scattering; Emergence of mass; Continuum Schwinger function methods; Dyson-Schwinger equations; STRUCTURE FUNCTIONS G(1)(P); DEEP-INELASTIC-SCATTERING; MUON-PROTON; NUCLEON; QUARK; QCD; Q(2)-DEPENDENCE; AMPLITUDES; DEPENDENCE; ASYMMETRY;
D O I
10.1016/j.physletb.2023.138074
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Supposing there exists an effective charge which defines an evolution scheme for both unpolarised and polarised parton distribution functions (DFs) that is all-orders exact and using Ansatze for hadron-scale proton polarised valence quark DFs, constrained by flavour-separated axial charges and insights from perturbative quantum chromodynamics, predictions are delivered for all proton polarised DFs at the scale & zeta;C2= 3 GeV2. The pointwise behaviour of the predicted DFs and, consequently, their moments, compare favourably with results inferred from data. Notably, flavour-separated singlet polarised DFs are small. On the other hand, the polarised gluon DF, ⠃G(x; & zeta;C), is large and positive. Using our result, we predict f10.05 dx ⠃G(x; & zeta;C) = 0.214(4) and that experimental measurements of the proton flavour-singlet axial charge should return aE0(& zeta;C) = 0.33(2).& COPY; 2023 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons .org /licenses /by /4 .0/). Funded by SCOAP3.
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页数:7
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