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Evaluation of \alpha (M^2_Z) and (g-2)_\mu

Abstract

This talk summarizes the recent development in the evaluation of the leading order hadronic contributions to the running of the QED fine structure constant \alpha(s), at s=MZ2s=M_{\rm Z}^2, and to the anomalous magnetic moments of the muon (g−2)μ(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 τ\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: Δαhad(M2Z)=(276.3±1.6)×10−4\Delta\alpha_{had} (M_2^Z) =(276.3\pm1.6)\times10^{-4}, yielding α−1(MZ2)=128.933±0.021\alpha^{-1}(M_{\rm Z}^2)=128.933\pm0.021, and aμhad=(692.4±6.2)×10−10a_\mu^{\rm had}=(692.4\pm6.2)\times 10^{-10} with which one finds for the complete Standard Model prediction aμSM=(11659159.6±6.7)×10−10a_\mu^{\rm SM}=(11 659 159.6\pm6.7)\times10^{-10}. For the electron (g−2)e(g-2)_e, the hadronic contribution is aehad=(187.5±1.8)×10−14a_e^{\rm had}=(187.5\pm1.8)\times 10^{-14}.Comment: 9 pages, Talk given at the ICHEP'98 Conference, Vancouver, Canada, July 23-29, 199

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