Reevaluation of the hadronic vacuum polarisation contributions to the Standard Model predictions of the muon g-2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$g-2$$\end{document} and α(mZ2)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\alpha (m_Z^2)}$$\end{document} using newest hadronic cross-section data

被引:0
|
作者
M. Davier
A. Hoecker
B. Malaescu
Z. Zhang
机构
[1] IN2P3-CNRS et Université Paris-Sud 11,Laboratoire de l’Accélérateur Linéaire
[2] CERN,Laboratoire de Physique Nucléaire et des Hautes Energies
[3] IN2P3-CNRS et Universités Pierre-et-Marie-Curie et Denis-Diderot,undefined
来源
The European Physical Journal C | 2017年 / 77卷 / 12期
关键词
D O I
10.1140/epjc/s10052-017-5161-6
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摘要
We reevaluate the hadronic vacuum polarisation contributions to the muon magnetic anomaly and to the running of the electromagnetic coupling constant at the Z-boson mass. We include newest e+e-→hadrons\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^+e^- \rightarrow \mathrm{hadrons}$$\end{document} cross-section data (among others) from the BABAR and VEPP-2000 experiments. For the muon (g-2)/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(g-2)/2$$\end{document} we find for the lowest-order hadronic contribution (693.1±3.4)×10-10\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(693.1 \pm 3.4)\times 10^{-10}$$\end{document}, improving the precision of our previous evaluation by 21%. The full Standard Model prediction differs by 3.5σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$3.5\,\sigma $$\end{document} from the experimental value. The five-quark hadronic contribution to α(mZ2)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha (m_Z^2)$$\end{document} is evaluated to be (276.0±0.9)×10-4\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(276.0\pm 0.9)\times 10^{-4}$$\end{document}.
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