{ "id": "hep-ph/9812370", "version": "v2", "published": "1998-12-15T15:32:58.000Z", "updated": "1998-12-17T10:01:31.000Z", "title": "Evaluation of $α(M_{\\rm Z}^2)$ and $(g-2)_μ$", "authors": [ "Michel Davier" ], "comment": "13 pages", "journal": "Nucl.Phys.Proc.Suppl. 76 (1999) 327-338", "doi": "10.1016/S0920-5632(99)00486-7", "categories": [ "hep-ph" ], "abstract": "This talk summarizes the recent developments in the evaluation of the leading order hadronic contributions to the running of the QED fine structure constant $\\alpha(s)$, at $s=M_{\\rm Z}^2$, and to the anomalous magnetic moment of the muon $(g-2)_\\mu$. The accuracy of the theoretical prediction of these observables is limited by the uncertainties on the hadronic contributions. Significant improvement has been achieved in a series of new analyses which is presented historically in three steps: (I), use of $\\tau$ spectral functions in addition to $e^+e^-$ cross sections, (II), extended use of perturbative QCD and (III), application of QCD sum rule techniques. The most precise values obtained are: $\\Delta\\alpha_{\\rm had}(M_{\\rm Z}^2)$, $=(276.3\\pm1.6)\\times10^{-4}$, yielding $\\alpha^{-1}(M_{\\rm Z}^2)=128.933\\pm0.021$, and $a_\\mu^{\\rm had}=(692.4\\pm6.2)\\times 10^{-10}$ with which one finds for the complete Standard Model prediction $a_\\mu^{\\rm SM}=(11 659 159.6\\pm6.7)\\times10^{-10}$. For the electron $(g-2)_e$, the hadronic contribution is $a_e^{\\rm had}=(187.5\\pm1.8)\\times 10^{-14}$.", "revisions": [ { "version": "v2", "updated": "1998-12-17T10:01:31.000Z" } ], "analyses": { "keywords": [ "evaluation", "complete standard model prediction", "qcd sum rule techniques", "leading order hadronic contributions", "qed fine structure constant" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 13, "language": "en", "license": "arXiv", "status": "editable", "inspire": 480952 } } }