2PI effective action and evolution equations of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\mathcal{N} = 4$\end{document} super Yang–Mills

被引：0

作者：

Jelena Smolic

Milena Smolic

机构：

[1] University of Amsterdam,Institute for Theoretical Physics

来源：

The European Physical Journal C | 2012年 / 72卷 / 8期

关键词：

Gauge Theory; Ghost; Effective Action; Transport Coefficient; Black Hole Formation;

D O I：

10.1140/epjc/s10052-012-2106-y

中图分类号：

学科分类号：

摘要：

We employ nPI effective action techniques to study \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\mathcal{N}=4$\end{document} super Yang–Mills, and write down the 2PI effective action of the theory to two-loop order in the symmetric phase. We also supply the evolution equations of two-point correlators within the theory.

引用

共 34 条

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[2] Strings in Flat Space and Plane Waves from \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\mathcal{N}} = 4$$\end{document} Super Yang Mills
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The European Physical Journal C - Particles and Fields, 2005, 39 (Suppl 3) : 27 - 30
[4] Study of multi-muon events produced in \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$p\bar{p}$\end{document} interactions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\sqrt{s}=1.96$\end{document} TeV
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[5] Dyson–Schwinger equations and N=4\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal{N}=4$$\end{document} SYM in Landau gauge
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[7] Note on the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $N=2$\end{document} super Yang-Mills gauge theory in a noncommutative differential geometry
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[9] Renormalization aspects of N=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal {N}=1$$\end{document} Super Yang–Mills theory in the Wess–Zumino gauge
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