Abstract

Phase shifts for $s$-wave $\pi\pi$ scattering in both the $I=0$ and $I=2$ channels are determined from a lattice QCD calculation performed on 741 gauge configurations obeying G-parity boundary conditions with a physical pion mass and lattice size of $32^3\times 64$. These results support our recent study of direct CP violation in $K\to\pi\pi$ decay \cite{Abbott:2020hxn}, improving our earlier 2015 calculation \cite{Bai:2015nea}. The phase shifts are determined for both stationary and moving $\pi\pi$ systems, at three ($I=0$) and four ($I=2$) different total momenta. We implement several $\pi\pi$ interpolating operators including a scalar bilinear "$\sigma$" operator and paired single-pion bilinear operators with the constituent pions carrying various relative momenta. Several techniques, including correlated fitting and a bootstrap determination of p-values have been used to refine the results and a comparison with the generalized eigenvalue problem (GEVP) method is given. A detailed systematic error analysis is performed which allows phase shift results to be presented at a fixed energy.

Highlights

  • The scattering of two pions is one of the simplest hadronic processes in QCD

  • Phase shifts for s-wave ππ scattering in both the I 1⁄4 0 and I 1⁄4 2 channels are determined from a lattice QCD calculation performed on 741 gauge configurations obeying G-parity boundary conditions with a physical pion mass and lattice size of 323 × 64

  • We report the first lattice QCD calculation of both I 1⁄4 0 and I 1⁄4 2 s-wave ππ phase shifts performed over a range of two-pion energies with a physical pion mass so that a chiral extrapolation is no longer necessary

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Summary

INTRODUCTION

The scattering of two pions is one of the simplest hadronic processes in QCD. Since the only meson involved, the pion, is the lightest hadron in the standard model and originates from the vacuum breaking of almost exact SUð2ÞL × SUð2ÞR chiral symmetry, the behavior of this process at low energy can be well described by chiral perturbation theory (ChPT) [1]. IV and V we present in detail our fitting procedures and results for single pion and ππ energies and two-point function amplitudes, together with a brief comparison with another data analysis method, the generalized eigenvalue problem

DESCRIPTION OF THE GAUGE ENSEMBLE
Ensemble generation
Ensemble properties
G-parity boundary conditions
OVERVIEW OF THE MEASUREMENTS
Interpolating operators
Momentum decomposition
Total momentum
Angular momentum
T2 A1 A1 A1
Matrix of two-point correlation functions
Contraction diagrams
Estimating statistical errors and goodness of fit
SINGLE PION ENERGIES AND MASS
FINITE-VOLUME ππ ENERGIES
Stationary frame
Moving frame
Normalized determinant
Comparison of multioperator multistate fits with the GEVP method
DETERMINATION OF THE PHASE SHIFT
Calculation technique
Lellouch-Lüscher factor
SYSTEMATIC ERROR ANALYSIS
Cubic symmetry breaking
Finite lattice spacing
Finite volume
Unphysical kinematics
Higher partial wave correction
Method
Excited state contamination
Error budget
VIII. CONCLUSIONS
Findings
Pion operator
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