Abstract

We calculate the s-wave pion–pion scattering length in the isospin I=2 channel in lattice QCD for pion masses ranging from 270 MeV to 485 MeV using two flavors of maximally twisted mass fermions at a lattice spacing of 0.086 fm. Additionally, we check for lattice artifacts with one calculation at a finer lattice spacing of 0.067 fm. We use chiral perturbation theory at next-to-leading order to extrapolate our results. At the physical pion mass, we find mπaππI=2=−0.04385(28)(38) for the scattering length, where the first error is statistical and the second is our estimate of several systematic effects.

Highlights

  • In the limit of massless up and down quarks, the resulting chiral symmetry of QCD is spontaneously broken and the meson spectrum contains three massless Goldstone bosons, π ± and π 0

  • Due to the unique role played by the pions, their interactions are strongly determined by the underlying chiral symmetry, and the s-wave pion–pion scattering lengths even vanish in the chiral limit

  • The pion masses ranged from 270 MeV to 485 MeV and the lattice spacing was a = 0.086 fm

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Summary

Introduction

In the limit of massless up and down quarks, the resulting chiral symmetry of QCD is spontaneously broken and the meson spectrum contains three massless Goldstone bosons, π ± and π 0. Due to the unique role played by the pions, their interactions are strongly determined by the underlying chiral symmetry, and the s-wave pion–pion scattering lengths even vanish in the chiral limit. The scattering lengths are sensitive to the chiral dynamics of the strong interactions, and the non-perturbative calculation thereof, the subject of this Letter, is an integral part of understanding the low energy properties of QCD. The masses of the quarks are not zero but small and induce an explicit but weak breaking of chiral symmetry. The pions are not massless but light. This breaking of chiral symmetry is systematically treated in chiral perturbation theory (χ PT) by considering the quark masses as perturbations

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