Abstract

We study isospin-1 P-wave $\pi\pi$ scattering in lattice QCD with two flavours of O($a$) improved Wilson fermions. For pion masses ranging from $m_\pi=265$ MeV to $m_\pi=437$ MeV, we determine the energy spectrum in the centre-of-mass frame and in three moving frames. We obtain the scattering phase shifts using L\"uscher's finite-volume quantisation condition. Fitting the dependence of the phase shifts on the scattering momentum to a Breit-Wigner form allows us to determine the resonance parameters $m_\rho$ and $g_{\rho\pi\pi}$. By combining the scattering phase shifts with the decay matrix element of the vector current, we calculate the timelike pion form factor, $F_\pi$, and compare the results to the Gounaris-Sakurai representation of the form factor in terms of the resonance parameters. In addition, we fit our data for the form factor to the functional form suggested by the Omn\`es representation, which allows for the extraction of the charge radius of the pion. As a further application, we discuss the long-distance behaviour of the vector correlator, which is dominated by the two-pion channel. We reconstruct the long-distance part in two ways: one based on the finite-volume energies and matrix elements and the other based on $F_\pi$. It is shown that this part can be accurately constrained using the reconstructions, which has important consequences for lattice calculations of the hadronic vacuum polarisation contribution to the muon anomalous magnetic moment.

Highlights

  • The study of hadronic resonances in terms of the underlying theory of QCD necessitates a nonperturbative treatment

  • Our spectra have been determined using the variational method for a total of eight different irreps in the center-of-mass frame and three different moving frames with lattice momenta up to d2 1⁄4 3

  • We have studied the consistency of different parametrizations of the phase shift by comparing the results for the mass mρ and the coupling gρππ obtained from fits to either the Breit-Wigner or the Gounaris-Sakurai representation

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Summary

INTRODUCTION

The study of hadronic resonances in terms of the underlying theory of QCD necessitates a nonperturbative treatment. An interesting and increasingly relevant application of lattice calculations of Fπ arises in the context of ab initio determinations of the hadronic vacuum polarization (HVP) contribution to the muon’s anomalous magnetic moment, ahμvp. The latter is accessible via the (spatially summed) vector correlator Gðx0Þ [23,24,25], which, at large Euclidean times x0 is dominated by the two-pion channel. The outline of this paper is as follows: In Sec. II we summarize the methods used for determining the isospin-1 scattering phase shift and the timelike pion form factor from our lattice calculations. Our analysis supersedes previous preliminary results presented in [27,28]

Determination of the finite volume energy spectrum
The distillation method
Gauge field configurations and distillation schemes
THE ρ RESONANCE
Energy spectra
THE TIMELIKE PION FORM FACTOR
HADRONIC VACUUM POLARIZATION
CONCLUSIONS
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