Abstract

We present the first calculation of the electromagnetic form factor of the $\pi$ meson at physical light quark masses. We use configurations generated by the MILC collaboration including the effect of $u$, $d$, $s$ and $c$ sea quarks with the Highly Improved Staggered Quark formalism. We work at three values of the lattice spacing on large volumes and with $u$/$d$ quark masses going down to the physical value. We study scalar and vector form factors for a range in space-like $q^2$ from 0.0 to -0.1 $\mathrm{GeV}^2$ and from their shape we extract mean square radii. Our vector form factor agrees well with experiment and we find $\langle r^2 \rangle_V = 0.403(18)(6) \,\mathrm{fm}^2$. For the scalar form factor we include quark-line disconnected contributions which have a significant impact on the radius. We give the first results for SU(3) flavour-singlet and octet scalar mean square radii, obtaining: $\langle r^2 \rangle_S^{\mathrm{singlet}} = 0.506(38)(53) \mathrm{fm}^2$ and $\langle r^2 \rangle_S^{\mathrm{octet}} = 0.431(38)(46) \mathrm{fm}^2$. We discuss the comparison with expectations from chiral perturbation theory.

Highlights

  • The electromagnetic form factor of the charged π meson parametrizes the deviations from the behavior of a pointlike particle when struck by a photon

  • We present the first calculation of the electromagnetic form factor of the π meson at physical light quark masses

  • The calculation for the connected scalar form factor proceeds in an identical way to that of the vector form factor discussed in Sec

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Summary

Introduction

The electromagnetic form factor of the charged π meson parametrizes the deviations from the behavior of a pointlike particle when struck by a photon. The experimental error is 1–1.5% in the region up to jq2j 1⁄4 0.1 GeV2 and so a lattice QCD calculation of the form factor there can provide a stringent test of QCD. This is complementary to tests of QCD through calculation of meson masses and of decay constants that parametrize meson annihilation, for example to a W boson [2,3].

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