Abstract

We deliver lattice results for the $I=0$ $\pi\pi$ elastic $s$-wave scattering length calculated with the MILC $N_f=3$ flavors of the Asqtad-improved staggered fermions. The scattering phase shifts are determined by L\"uscher's formula from the energy-eigenvalues of $\pi\pi$ systems at one center of mass frame and four moving frames using the moving wall source technique. Our measurements are good enough to resolve the scattering length $a$ and effective range $r$, moreover, it allows us to roughly estimate the shape parameter $P$. Using our lattice results, the scattering length $a$ and effective range $r$ at the physical point are extrapolated by chiral perturbation theory. Our results are reasonably consistent with the Roy equation determinations and the newer experimental data. Numerical computations are carried out with two MILC fine ($a\approx0.09$~fm, $L^3 \times T = 40^3\times 96$) and one MILC superfine ($a\approx0.06$~fm, $L^3 \times T = 48^3\times 144$) lattice ensembles at three pion masses of $m_\pi\sim247~{\rm MeV}$, $249~{\rm MeV}$, and $314~{\rm MeV}$, respectively.

Highlights

  • The pion-pion scattering amplitudes are solely predicted at leading order (LO) in chiral perturbation theory [1]

  • The next-to-leading order (NLO) and next-to-next-to-leading order (NNLO) corrections in the chiral expansion result in the perturbative deviations from the LO prediction for small pion masses, and include both estimable nonanalytical contributions and analytical terms with low-energy constants (LEC’s) [2,3,4,5,6], which can be secured from the experimental measurements or lattice calculations

  • Extrapolated to the physical value of mπ=fπ, our final results give rise to mπaI01⁄40 1⁄4 0.217ð9Þð5Þ; lπI1⁄4π 0 1⁄4 45.6ð7.6Þð3.8Þ; which are in reasonable agreement with the recent experimental and theoretical determinations as well as the lattice calculations available in the literature

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Summary

INTRODUCTION

The pion-pion (ππ) scattering amplitudes are solely predicted at leading order (LO) in chiral perturbation theory (χPT) [1]. Using Roy equations after the correction for isospin breaking mass effects, the NA48=2 decisive analyses of the Ke4 and K3π decays lead to the robust results on the s-wave ππ scattering lengths [8]. All of these values can be used to inversely determine the significant values of the LEC’s.

FINITE-VOLUME METHODS
Center-of-mass frame
Moving frame
Lattice calculation
Extraction of energies
FITTING ANALYSES
The effective range approximation parameters
CHIRAL EXTRAPOLATIONS
Threshold parameters in χ PT
Chiral extrapolation of threshold parameters
SUMMARY AND CONCLUSION
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