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Hadronic vacuum polarization: $(g-2)_\mu$ versus global electroweak fits

High Energy Physics - Phenomenology 2020-08-31 v3 High Energy Physics - Experiment High Energy Physics - Lattice Nuclear Experiment Nuclear Theory

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 (g2)μ(g-2)_\mu, 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)\Delta\alpha^{(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)×104\Delta \alpha^{(5)}_\text{had}\big|_\text{EW}=270.2(3.0)\times 10^{-4}. This value actually lies below the range derived from e+ehadronse^+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 (g2)μ(g-2)_\mu 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 (g2)μ(g-2)_\mu by adjusting HVP would thus not necessarily weaken the case for physics beyond the SM (BSM), but to some extent shift it from (g2)μ(g-2)_\mu to the EW fit. We briefly explore some options of BSM scenarios that could conceivably explain the ensuing tension.

Keywords

Cite

@article{arxiv.2003.04886,
  title  = {Hadronic vacuum polarization: $(g-2)_\mu$ versus global electroweak fits},
  author = {Andreas Crivellin and Martin Hoferichter and Claudio Andrea Manzari and Marc Montull},
  journal= {arXiv preprint arXiv:2003.04886},
  year   = {2020}
}

Comments

7 pages, 2 figures; journal version

R2 v1 2026-06-23T14:10:34.128Z