Hadronic vacuum polarization: (g−2)μ(g-2)_μ versus global electroweak fits

preprint2020arXivOpen access

Abstract

Hadronic vacuum polarization (HVP) is not only a critical part of the Standard Model (SM) prediction for the anomalous magnetic moment of the muon (g−2)μ(g-2)_μ, but also a crucial ingredient for global fits to electroweak (EW) precision observables due to its contribution to the running of the fine-structure constant encoded in Δαhad(5)Δα^{(5)}_\text{had}. We find that with modern EW precision data, including the measurement of the Higgs mass, the global fit alone provides a competitive, independent determination of Δαhad(5)∣EW=270.2(3.0)×10−4Δα^{(5)}_\text{had}\big|_\text{EW}=270.2(3.0)\times 10^{-4}. This value actually lies below the range derived from e+e−→hadronse^+e^-\to\text{hadrons} cross-section data, and thus goes into the opposite direction as would be required if a change in HVP were to bring the SM prediction for (g−2)μ(g-2)_μ into agreement with the Brookhaven measurement. Depending on the energy where the bulk of the changes in the cross section occurs, reconciling experiment and SM prediction for (g−2)μ(g-2)_μ by adjusting HVP would thus not necessarily weaken the case for physics beyond the SM (BSM), but to some extent shift it from (g−2)μ(g-2)_μ to the EW fit. We briefly explore some options of BSM scenarios that could conceivably explain the ensuing tension.

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