We present a comprehensive study of the electromagnetic form factor, the decay constant and the mass of the pion computed in lattice QCD with two degenerate O(a)-improved Wilson quarks at three different lattice spacings in the range 0:05-0:08 fm and pion masses between 280 and 630 MeV at m π L ≥ 4. Using partially twisted boundary conditions and stochastic estimators, we obtain a dense set of precise data points for the form factor at very small momentum transfers, allowing for a model-independent extraction of the charge radius. Chiral Perturbation Theory (ChPT) augmented by terms which model lattice artefacts is then compared to the data. At next-to-leading order the effective theory fails to produce a consistent description of the full set of pion observables but describes the data well when only the decay constant and mass are considered. By contrast, using the next-to-next-to-leading order expressions to perform global fits result in a consistent description of all data. We obtain 〈rπ2〉 = 0:481(33)(13) fm2 as our final result for the charge radius at the physical point. Our calculation also yields estimates for the pion decay constant in the chiral limit, Fπ/F = 1:080(16)(6), the quark condensate, Σ1/3/MS(2 GeV) = 261(13)(1) MeV and several low-energy constants of SU(2) ChPT. © SISSA 2013.
CITATION STYLE
Brandt, B. B., Jüttner, A., & Wittig, H. (2013). The pion vector form factor from lattice QCD and NNLO chiral perturbation theory. Journal of High Energy Physics, 2013(11). https://doi.org/10.1007/JHEP11(2013)034
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