MSSM corrections to the top–antitop quark forward–backward asymmetry at the Tevatron

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作者
Stefan Berge
Doreen Wackeroth
Martin Wiebusch
机构
[1] Johannes Gutenberg-Universität,PRISMA Cluster of Excellence, Institute for Physics (WA THEP)
[2] University at Buffalo,Department of Physics
[3] The State University of New York,Institute for Theoretical Particle Physics
[4] Karlsruhe Institute of Technology (KIT),undefined
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Minimal Supersymmetric Standard Model; Loop Function; Minimal Flavor Violation; Squark Masse; Neutralino Mass;
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摘要
We study the effects of the complete supersymmetric QCD and electroweak one-loop corrections to the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$t\bar{t}$\end{document} forward–backward asymmetry at the Fermilab Tevatron \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} collider. We work in the complex Minimal Supersymmetric Standard Model (MSSM), only restricted by the condition of minimal flavor violation (MFV). We perform a comprehensive scan over the relevant parameter space of the complex MFV–MSSM and determine the maximal possible contributions of these MSSM loop corrections to the forward–backward asymmetry in the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$t\bar{t}$\end{document} center-of-mass frame. We find that the SUSY loop-induced asymmetry at the Tevatron with \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$M_{t\bar{t}}>450~\mbox{GeV}$\end{document} can be at most +2 % for very light SUSY particles, i.e. for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$m_{\tilde{t}_{1}} <100~\mbox{GeV}$\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}$m_{\min} = \mathrm{Min}\{ m_{\tilde{g}},m_{\tilde{u}_{1,2}},m_{\tilde{d}_{1,2}}\}<100~\mbox{GeV}$\end{document}, which reduces to 0.1 % for gluino and squark masses in the range 850 GeV–1000 GeV and a light top squark of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$m_{\tilde{t}_{1}}=200~\mbox{GeV}$\end{document}.
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