Abstract

The π^{0} pole constitutes the lowest-lying singularity of the hadronic light-by-light (HLBL) tensor, and thus, it provides the leading contribution in a dispersive approach to HLBL scattering in the anomalous magnetic moment of the muon (g-2)_{μ}. It is unambiguously defined in terms of the doubly virtual pion transition form factor, which in principle, can be accessed in its entirety by experiment. We demonstrate that, in the absence of a direct measurement, the full spacelike doubly virtual form factor can be reconstructed very accurately based on existing data for e^{+}e^{-}→3π, e^{+}e^{-}→e^{+}e^{-}π^{0}, and the π^{0}→γγ decay width. We derive a representation that incorporates all the low-lying singularities of the form factor, matches correctly onto the asymptotic behavior expected from perturbative QCD, and is suitable for the evaluation of the (g-2)_{μ} loop integral. The resulting value, a_{μ}^{π^{0}-pole}=62.6_{-2.5}^{+3.0}×10^{-11}, for the first time, represents a complete data-driven determination of the pion-pole contribution with fully controlled uncertainty estimates. In particular, we show that already improved singly virtual measurements alone would allow one to further reduce the uncertainty in a_{μ}^{π^{0}-pole}.

Highlights

  • Introduction.—The anomalous magnetic moment of the muon ðg − 2Þμ constitutes a highly sensitive probe of physics beyond the Standard Model (BSM)

  • The π0 pole constitutes the lowest-lying singularity of the hadronic light-by-light (HLBL) tensor, and it provides the leading contribution in a dispersive approach to HLBL scattering in the anomalous magnetic moment of the muon ðg − 2Þμ

  • Its value is dominated by the final report of the BNL E821 experiment [1], which departs from the SM by about 3σ, and adds to the intriguing hints for BSM physics observed in the muon sector

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Summary

Introduction

Introduction.—The anomalous magnetic moment of the muon ðg − 2Þμ constitutes a highly sensitive probe of physics beyond the Standard Model (BSM). Martin Hoferichter,1 Bai-Long Hoid,2 Bastian Kubis,2 Stefan Leupold,3 and Sebastian P.

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