Abstract
We present an investigation of the electromagnetic pion form factor, $F_\pi(Q^2)$, at small values of the four-momentum transfer $Q^2$ ($\lesssim 0.25$ GeV$^2$), based on the gauge configurations generated by European Twisted Mass Collaboration with $N_f = 2$ twisted-mass quarks at maximal twist including a clover term. Momentum is injected using non-periodic boundary conditions and the calculations are carried out at a fixed lattice spacing ($a \simeq 0.09$ fm) and with pion masses equal to its physical value, 240 MeV and 340 MeV. Our data are successfully analyzed using Chiral Perturbation Theory at next-to-leading order in the light-quark mass. For each pion mass two different lattice volumes are used to take care of finite size effects. Our final result for the squared charge radius is $\langle r^2 \rangle_\pi = 0.443~(29)$ fm$^2$, where the error includes several sources of systematic errors except the uncertainty related to discretization effects. The corresponding value of the SU(2) chiral low-energy constant $\overline{\ell}_6$ is equal to $\overline{\ell}_6 = 16.2 ~ (1.0)$.
Highlights
The investigation of the physical properties of the pion, which is the lightest bound state in quantum chromodynamics (QCD), can provide crucial information on the way low-energy dynamics is governed by the quark and gluon degrees of freedom
We present an investigation of the electromagnetic pion form factor, FπðQ2Þ, at small values of the fourmomentum transfer Q2 (≲0.25 GeV2), based on the gauge configurations generated by the European Twisted Mass Collaboration with Nf 1⁄4 2 twisted-mass quarks at maximal twist including a clover term
Our final result for the squared charge radius is hr2iπ 1⁄4 0.443ð29Þ fm2, where the error includes several sources of systematic errors except the uncertainty related to discretization effects
Summary
The investigation of the physical properties of the pion, which is the lightest bound state in quantum chromodynamics (QCD), can provide crucial information on the way low-energy dynamics is governed by the quark and gluon degrees of freedom The determination of FπðQ2Þ from lattice QCD simulations provides an excellent opportunity for the study of chiral logarithms The latter are important in the case of the squared pion charge radius r2π, i.e., the slope of pion form factor at Q2 1⁄4 0.
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