Abstract

We show that using renormalization-group summation to generate the QCD radiative corrections to the $\pi-\gamma$ transition form factor, calculated with lightcone sum rules (LCSR), renders the strong coupling free of Landau singularities while preserving the QCD form-factor asymptotics. This enables a reliable applicability of the LCSR method to momenta well below 1 GeV$^2$. This way, one can use the new preliminary BESIII data with unprecedented accuracy below 1.5 GeV$^2$ to fine tune the prefactor of the twist-six contribution. Using a combined fit to all available data below 3.1 GeV$^2$, we are able to determine all nonperturbative scale parameters and a few Gegenbauer coefficients entering the calculation of the form factor. Employing these ingredients, we determine a pion distribution amplitude with conformal coefficients $(b_2,b_4)$ that agree at the $1\sigma$ level with the data for $Q^2 \leqslant 3.1$ GeV$^2$ and fulfill at the same time the lattice constraints on $b_2$ at N$^3$LO together with the constraints from QCD sum rules with nonlocal condensates.The form-factor prediction calculated herewith reproduces the data below 1 GeV$^2$ significantly better than analogous predictions based on a fixed-order power-series expansion in the strong coupling constant.

Highlights

  • A useful scheme to consider quantitatively exclusive reactions of hadrons in QCD is provided by the method of lightcone sum rules (LCSRs) in terms of a dispersion relation [1,2]

  • We show that using renormalization-group summation to generate the QCD radiative corrections to the π − γ transition form factor, calculated with light-cone sum rules (LCSR), renders the strong coupling free of Landau singularities while preserving the QCD form-factor asymptotics

  • The transition form factor (TFF) predictions obtained with the new fractional analytic perturbation theory (FAPT)/LCSR scheme are shown in comparison with a collection of data in a wider momentum region up to Q2 < 5.5 GeV2 in Sec

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Summary

INTRODUCTION

A useful scheme to consider quantitatively exclusive reactions of hadrons in QCD is provided by the method of lightcone sum rules (LCSRs) in terms of a dispersion relation [1,2]. The domain of applicability of the QCD perturbative expansion within the FAPT/LCSR approach is significantly extended toward lower momentum transfers allowing a comparison with the data within a more reliable margin of error. This is all the more important in the case of the preliminary BESIII data which bear below Q2 < 1.5 GeV2 an unprecedented accuracy [14]. The TFF predictions obtained with the new FAPT/LCSR scheme are shown in comparison with a collection of data in a wider momentum region up to Q2 < 5.5 GeV2 in Sec. V making it apparent that our approach works well even above the low-Q2 range used in the fit. The ERBL exponent incorporates all evolution kernels aksþ1Vk, whereas the partonic subprocesses, encoded in the coefficient functions aksT ðkÞ, are taken into account in terms of the leading-twist amplitude Tð2Þ

Main perturbative ingredients using RG summation
RG technique in connection with a dispersion relation
Pion-photon TFF in FAPT
About the role of NNLO corrections OðA2Þ to the TFF
TRANSITION FORM FACTOR WITHIN THE LCSR EMPLOYING ERBL SUMMATION
CONCLUSIONS
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