6533b86cfe1ef96bd12c8263

RESEARCH PRODUCT

Anomalous magnetic moment of the muon: A hybrid approach

N. F. NasrallahH. SpiesbergerH. SpiesbergerCesareo A. DominguezBenjamin JägerK. SchilcherK. SchilcherHanno HorchHartmut Wittig

subject

PhysicsQuantum chromodynamicsParticle physicsMuonAnnihilationAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Hadronhep-latFOS: Physical sciencesPerturbative QCDhep-phLattice QCD01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentSum rule in quantum mechanics010306 general physics

description

A new QCD sum rule determination of the leading order hadronic vacuum polarization contribution to the anomalous magnetic moment of the muon, $a_{\mu}^{\rm hvp}$, is proposed. This approach combines data on $e^{+}e^{-}$ annihilation into hadrons, perturbative QCD and lattice QCD results for the first derivative of the electromagnetic current correlator at zero momentum transfer, $\Pi_{\rm EM}^\prime(0)$. The idea is based on the observation that, in the relevant kinematic domain, the integration kernel $K(s)$, entering the formula relating $a_{\mu}^{\rm hvp}$ to $e^{+}e^{-}$ annihilation data, behaves like $1/s$ times a very smooth function of $s$, the squared energy. We find an expression for $a_{\mu}$ in terms of $\Pi_{\rm EM}^\prime(0)$, which can be calculated in lattice QCD. Using recent lattice results we find a good approximation for $a_{\mu}^{\rm hvp}$, but the precision is not yet sufficient to resolve the discrepancy between the $R(s)$ data-based results and the experimentally measured value.

https://doi.org/10.1103/physrevd.96.074016