Collins effect and single spin azimuthal asymmetriesin the HERMES and COMPASS experiments

被引:0
作者
A. V. Efremov
K. Goeke
P. Schweitzer
机构
[1] Joint Institute for Nuclear Research,Institut für Theoretische Physik II
[2] Ruhr-Universität Bochum,undefined
来源
The European Physical Journal C - Particles and Fields | 2003年 / 32卷
关键词
Distribution Function; Parton Distribution; Fragmentation Function; Parton Distribution Function; Pion Production;
D O I
暂无
中图分类号
学科分类号
摘要
Predictions are made for single spin azimuthal asymmetries due to the Collins effect in pion production from semi-inclusive deeply inelastic scattering off transversely and longitudinally polarized targets for the HERMES and COMPASS experiments. The x-dependence of the asymmetries is evaluated using the parton distribution functions from the chiral quark-soliton model. The overall normalization of the predicted asymmetries is determined by the information on the Collins fragmentation function extracted from previous HERMES data on azimuthal asymmetries \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$A_{\mathrm {{UL}}}^{\sin\phi}$\end{document} from a longitudinally polarized target. The single spin asymmetries AUT from the transversely polarized proton target are found to be about \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$20\%$\end{document} for positive and neutral pions both at HERMES and COMPASS. For a longitudinally polarized target we obtain for COMPASS \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$A_{\mathrm {{UL}}}^{\sin\phi}\sim 1\%$\end{document} and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$A_{\mathrm {{UL}}}^{\sin2\phi}\sim 3\%$\end{document}.
引用
收藏
页码:337 / 346
页数:9
相关论文
共 49 条
  • [1] Collaboration] undefined(1999)undefined Nucl. Phys. Proc. Suppl. 79 523-undefined
  • [2] Collaboration] undefined(2000)undefined Phys. Rev. Lett. 84 4047-undefined
  • [3] Collaboration] undefined(2001)undefined Phys. Rev. D 64 097101-undefined
  • [4] Collaboration] undefined(2003)undefined Phys. Lett. B 562 182-undefined
  • [5] Collaboration] undefined(1999)undefined Nucl. Phys. Proc. Suppl. 79 520-undefined
  • [6] Collins undefined(1993)undefined Nucl. Phys. B 396 161-undefined
  • [7] Sivers undefined(1990)undefined Phys. Rev. D 41 83-undefined
  • [8] Ralston undefined(1979)undefined Nucl. Phys. B 152 109-undefined
  • [9] Efremov undefined(1992)undefined Phys. Lett. B 284 394-undefined
  • [10] Collins undefined(2002)undefined Phys. Lett. B 536 43-undefined