The description of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$F_2$\end{document} at low \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$Q^2$\end{document}

被引:0
|
作者
A.D. Martin
M.G. Ryskin
A.M. Stasto
机构
[1] Department of Physics,
[2] University of Durham,undefined
[3] Durham,undefined
[4] DH1 3LE,undefined
[5] UK ,undefined
[6] Petersburg Nuclear Physics Institute,undefined
[7] 188350,undefined
[8] Gatchina,undefined
[9] St. Petersburg,undefined
[10] Russia ,undefined
[11] H. Niewodniczanski Institute of Nuclear Physics,undefined
[12] 31-342 Krakow,undefined
[13] Poland ,undefined
关键词
Structure Function; High Mass; Small Distance; Entire Domain; Mass State;
D O I
10.1007/s100529801035
中图分类号
学科分类号
摘要
We analyse the data for the proton structure function \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$F_2$\end{document} over the entire \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$Q^2$\end{document} domain, including especially low \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$Q^2$\end{document}, in terms of perturbative and non-perturbative QCD contributions. The small distance configurations are given by perturbative QCD, while the large distance contributions are given by the vector dominance model and, for the higher mass \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$q \overline{q}$\end{document} states, by the additive quark approach. The interference between states of different \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$q\bar{q}$\end{document} mass (in the perturbative contribution) is found to play a crucial role in obtaining an excellent description of the data throughout the whole \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$Q^2$\end{document} region, including photoproduction.
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页码:643 / 654
页数:11
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