TY - JOUR
T1 - The hadronic vacuum polarization contribution to the muon g − 2 from lattice QCD
AU - Della Morte, Michele
AU - Francis, Anthony
AU - Gulpers, Vera
AU - Gregorio, Herdoiza
AU - von Hippel, G.
AU - Hanno, Horch
AU - Jager, Benjamin
AU - Meyer, Harvey
AU - Nyffeler, A
AU - Wittig, Hartmut
PY - 2017
Y1 - 2017
N2 - We present a calculation of the hadronic vacuum polarization contribution to the muon anomalous magnetic moment, a
μ
hvp, in lattice QCD employing dynamical up and down quarks. We focus on controlling the infrared regime of the vacuum polarization function. To this end we employ several complementary approaches, including Padé fits, time moments and the time-momentum representation. We correct our results for finite-volume effects by combining the Gounaris-Sakurai parameterization of the timelike pion form factor with the Lüscher formalism. On a subset of our ensembles we have derived an upper bound on the magnitude of quark-disconnected diagrams and found that they decrease the estimate for a
μ
hvp by at most 2%. Our final result is aμhvp=(654±32−23+21)·10
−10, where the first error is statistical, and the second denotes the combined systematic uncertainty. Based on our findings we discuss the prospects for determining a
μ
hvp with sub-percent precision.
AB - We present a calculation of the hadronic vacuum polarization contribution to the muon anomalous magnetic moment, a
μ
hvp, in lattice QCD employing dynamical up and down quarks. We focus on controlling the infrared regime of the vacuum polarization function. To this end we employ several complementary approaches, including Padé fits, time moments and the time-momentum representation. We correct our results for finite-volume effects by combining the Gounaris-Sakurai parameterization of the timelike pion form factor with the Lüscher formalism. On a subset of our ensembles we have derived an upper bound on the magnitude of quark-disconnected diagrams and found that they decrease the estimate for a
μ
hvp by at most 2%. Our final result is aμhvp=(654±32−23+21)·10
−10, where the first error is statistical, and the second denotes the combined systematic uncertainty. Based on our findings we discuss the prospects for determining a
μ
hvp with sub-percent precision.
KW - Lattice QCD
KW - Nonperturbative Effects
KW - Precision QED
U2 - 10.1007/JHEP10(2017)020
DO - 10.1007/JHEP10(2017)020
M3 - Journal article
SN - 1126-6708
VL - 2017
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 10
M1 - 20
ER -