6533b81ffe1ef96bd12787d2

RESEARCH PRODUCT

Theoretical determination of the hadronic (g-2) of the muon

Hubert SpiesbergerHubert SpiesbergerKarl SchilcherKarl SchilcherCesareo A. Dominguez

subject

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMuonAnnihilation010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyPerturbative QCDOrder (ring theory)Astronomy and AstrophysicsLattice QCD01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentOperator product expansionAnomaly (physics)010306 general physics

description

An approach is discussed on the determination of the leading order hadronic contribution to the muon anomaly, $a_\mu^{HAD}$, based entirely on theory. This method makes no use of $e^+ e^-$ annihilation data, a likely source of the current discrepancy between theory and experiment beyond the $3\, \sigma$ level. What this method requires is essentially knowledge of the first derivative of the vector current correlator at zero-momentum. In the heavy-quark sector this is obtained from the well known heavy quark expansion in perturbative QCD, leading to values of $a_\mu^{HAD}$ in the charm- and bottom-quark region which were fully confirmed by later lattice QCD (LQCD) results. In the light-quark sector, using recent preliminary LQCD results for the first derivative of the vector current correlator at zero-momentum leads to the value $a_\mu^{HAD} = (729 - 871)\, \times\,10^{-10}$, which is significantly larger than values obtained from using $e^+ e^-$ data. A separate approach based on the operator product expansion (OPE), and designed to quench the contribution of these data, reduces the discrepancy by at least 40\%. In addition, it exposes a tension between the OPE and $e^+ e^-$ data, thus suggesting the blame for the discrepancy on the latter.

10.1142/s0217732316300354http://arxiv.org/abs/1605.07903