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Lattice calculation of the pion transition form factor with Nf=2+1N_f=2+1 Wilson quarks

Abstract

We present a lattice QCD calculation of the double-virtual neutral pion transition form factor, with the goal to cover the kinematic range relevant to hadronic light-by-light scattering in the muon g2g-2. Several improvements have been made compared to our previous work. First, we take into account the effects of the strange quark by using the Nf=2+1N_f=2+1 CLS gauge ensembles. Secondly, we have implemented the on-shell O(a)\mathcal{O}(a)-improvement of the vector current to reduce the discretization effects associated with Wilson quarks. Finally, in order to have access to a wider range of photon virtualities, we have computed the transition form factor in a moving frame as well as in the pion rest-frame. After extrapolating the form factor to the continuum and to physical quark masses, we compare our results with phenomenology. We extract the normalization of the form factor with a precision of 3.5\% and confirm within our uncertainty previous somewhat conflicting estimates for a low-energy constant that appears in chiral perturbation theory for the decay π0γγ\pi^0 \to \gamma\gamma at NLO. With additional input from experiment and theory, we reproduce recent estimates for the decay width Γ(π0γγ)\Gamma(\pi^0 \to \gamma\gamma). We also study the asymptotic large-Q2Q^2 behavior of the transition form factor in the double-virtual case. Finally, we provide as our main result a more precise model-independent lattice estimate of the pion-pole contribution to hadronic light-by-light scattering in the muon g2g-2: aμHLbL;π0=(59.7±3.6)×1011a_{\mu}^{\mathrm{HLbL}; \pi^0} = (59.7 \pm 3.6) \times 10^{-11}. Using in addition the normalization of the form factor obtained by the PrimEx experiment, we get the lattice and data-driven estimate aμHLbL;π0=(62.3±2.3)×1011a_{\mu}^{\mathrm{HLbL}; \pi^0} = (62.3 \pm 2.3) \times 10^{-11}.Comment: 29 pages, 14 figures. v2: minor corrections to match the published version. A file with the transition form factor data at the physical pion mass and in the continuum is included in the submissio

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