Hadronic-vacuum-polarization contribution to the muon's anomalous magnetic moment from four-flavor lattice QCD

We calculate the contribution to the muon anomalous magnetic moment hadronic vacuum polarization from the connected diagrams of up and down quarks, omitting electromagnetism. We employ QCD gauge-field configurations with dynamical u, d, s, and c quarks and the physical pion mass, and analyze five ensembles with lattice spacings ranging from a approximate to 0.06 to 0.15 fm. The up- and down-quark masses in our simulations have equal masses m(l). We obtain, in this world where all pions have the mass of the pi(0), 10(10)a(mu)(ll)(conn.) = 637.8(8.8), in agreement with independent lattice-QCD calculations. We then combine this value with published lattice-QCD results for the connected contributions from strange, charm, and bottom quarks, and an estimate of the uncertainty due to the fact that our calculation does not include strong-isospin breaking, electromagnetism, or contributions from quark-disconnected diagrams. Our final result for the total O(alpha(2)) hadronic-vacuum polarization to the muon's anomalous magnetic moment is 10(10)a(mu)(HVP,LO) = 699(15)(u,d) (1)(s,c,b), where the errors are from the light-quark and heavy-quark contributions, respectively. Our result agrees with both ab-initio lattice-QCD calculations and phenomenological determinations from experimental e(+) e(-)-scattering data. It is 1 .3 sigma below the "no new physics" value of the hadronic-vacuum-polarization contribution inferred from combining the BNL E821 measurement of a(mu) with theoretical calculations of the other contributions.