Hadronic contribution to the QED running coupling α(MZ2)α(M_{Z}^2)

preprint2012arXivOpen access

Abstract

We introduce a model independent method for the determination of the hadronic contribution to the QED running coupling, ΔαHAD(MZ2)Δα_{\text{HAD}}(M_{Z}^{2}), requiring no e+e−e^+e^- annihilation data as input. This is achieved by calculating the heavy-quark contributions entirely in perturbative QCD, whilst the light-quark resonance piece is determined using available lattice QCD results. Future reduction in the current uncertainties in the latter shall turn this method into a valuable alternative to the standard approach. Subsequently, we find that the precision of current determinations of ΔαHAD(MZ2)Δα_{\text{HAD}}(M_{Z}^{2}) can be improved by some 20% by computing the heavy-quark pieces in PQCD, whilst using e+e−e^+e^- data only for the low-energy light-quark sector. We obtain in this case ΔαHAD(MZ2)=275.7(0.8)×10−4Δα_{\text{HAD}}(M_{Z}^{2})=275.7(0.8) \times 10^{-4}, which currently is the most precise value of ΔαHAD(MZ2)Δα_{\text{HAD}}(M_{Z}^{2}).

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