Abstract

We report the first lattice QCD calculation of the hadronic vacuum polarization (HVP) disconnected contribution to the muon anomalous magnetic moment at physical pion mass. The calculation uses a refined noise-reduction technique that enables the control of statistical uncertainties at the desired level with modest computational effort. Measurements were performed on the 48^{3}×96 physical-pion-mass lattice generated by the RBC and UKQCD Collaborations. We find the leading-order hadronic vacuum polarization a_{μ}^{HVP(LO)disc}=-9.6(3.3)(2.3)×10^{-10}, where the first error is statistical and the second systematic.

Highlights

  • We report the first lattice quantum chromodynamics (QCD) calculation of the hadronic vacuum polarization (HVP) disconnected contribution to the muon anomalous magnetic moment at physical pion mass

  • New physics contributions to al are expected to scale as al − aSlM ∝ ðm2l=Λ2NPÞ for lepton l 1⁄4 e, μ, τ and new physics scale ΛNP

  • The current standard model (SM) prediction for the hadronic light-by-light (HLBL) contribution [11] is based on a model of quantum chromodynamics (QCD); important progress towards a first-principles computation has been made recently [12,13,14]

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Summary

Electroweak corrections

AHμ VP ðLOÞ disc at physical pion mass. We report the result for the combined up, down, and strange-quark contributions. The current SM prediction for the HLBL contribution [11] is based on a model of quantum chromodynamics (QCD); important progress towards a first-principles computation has been made recently [12,13,14]. One of the main challenges in the first-principles computation of the HVP contribution with percent or subpercent uncertainties is the control of statistical noise for the quark-disconnected contribution (see Fig. 1) at physical pion mass. Significant progress has been made recently in the computation of an upper bound [15,16,17], an estimate using lattice QCD data at heavy pion mass [18], and towards a first-principles computation at physical pion mass [19]. We compute Πðq2Þ using the kernel function of Refs. [21,22], Πðq2Þ

XcosðqtÞ t
PHYSICAL f μ ðtÞ
Sparse grid spacing N
We now define the partial sums

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