Precise determination of the low-energy hadronic contribution to the muon from analyticity and unitarity: An improved analysis
arXiv:1605.00202 · doi:10.1103/PhysRevD.93.116007
Abstract
The two-pion low-energy contribution to the anomalous magnetic moment of the muon, , expres sed as an integral over the modulus squared of the pion electromagnetic form fac tor, brings a relatively large contribution to the theoretical error, since the low accuracy of experimental measurements in this region is amplified by the drastic increase of the integration kernel. We derive stringent constraints on the two-pion contribution by exploiting analyticity and unitarity of the pion electromagnetic form factor. To avoid the poor knowledge of the modulus of this function, we use instead its phase, known with high precision in the elastic region from Roy equations for pion-pion scattering via the Fermi-Watson theorem. Above the inelastic threshold we adopt a conservative integral condition on the modulus, determined from data and perturbative QCD. Additional high precision data on the modulus in the range GeV, obtained from annihilation and -decay experiments, are used to improve the predictions on the modulus at lower energies by means of a parametrization-free analytic extrapolation. The results are optimal for a given input and do not depend on the unknown phase of the form factor above the inelastic threshold. The present work improves a previous analysis based on the same technique, including more experimental data and employing better statistical tools for their treatment. We obtain for the contribution to from below 0.63 GeV the value , which amounts to a reduction of the theoretical error by about .
13 pages, latex using revtex 4, 8 figures; revised version includes two additional references, improved discussions, figures touched up
References in corpus (12)
- The pion-pion scattering amplitude. IV: Improved analysis with once subtracted Roy-like equations up to 1100 MeV
- Muon g-2: Review of Theory and Experiment
- Determination of the Charged Pion Form Factor at Q2=1.60 and 2.45 (GeV/c)2
- Charged pion form factor between Q^2=0.60 and 2.45 GeV^2. II. Determination of, and results for, the pion form factor
- Update of the e^+e^-\toπ^+π^- cross section measured by SND detector in the energy region 400<\sqrt{s}<1000 MeV
- Measurement of sigma(e+ e- -> pi+ pi-) from threshold to 0.85 GeV^2 using Initial State Radiation with the KLOE detector
- A new approach to evaluate the leading hadronic corrections to the muon g-2
- Measurement of the e+e- -> pi+pi- cross section with the CMD-2 detector in the 370-520 MeV c.m. energy range
- Long-distance radiative corrections to the di-pion tau lepton decay
- Measurement of the cross section in the center-of-mass energy range 1.22--2.00 GeV with the SND detector at the VEPP-2000 collider
- Spacelike pion form factor from analytic continuation and the onset of perturbative QCD
- Model independent bounds on the modulus of the pion form factor on the unitarity cut below the threshold
Cited by in corpus (11)
- The of charged leptons, and the hyperfine splitting of muonium
- Kaon electromagnetic form factors in dispersion theory
- Isospin-breaking effects in the two-pion contribution to hadronic vacuum polarization
- Radiative resonance couplings in
- Electromagnetic charge radius of the pion at high precision
- Dispersion relations for the hadronic VVA correlator
- Test of analyticity and unitarity for the pion form-factor data around the resonance
- A Simple Parametrisation of the Pion Form Factor
- Study of pion vector form factor and its contribution to the muon
- Momentum-dependence of mixing in the pion vector form factor and its effect on
- Structure-dependent radiative corrections to in the GVMD approach