Abstract

We derive the light-front wave function (LFWF) representation of the $\gamma^* \gamma^* \to \eta_c(1S)\,,\eta_c(2S)$ transition form factor $F(Q_1^2, Q_2^2)$ for two virtual photons in the initial state. For the LFWF, we use different models obtained from the solution of the Schr\"odinger equation for a variety of $c \bar c$ potentials. We compare our results to the BaBar experimental data for the $\eta_c(1S)$ transition form factor, for one real and one virtual photon. We observe that the onset of the asymptotic behaviour is strongly delayed and discuss applicability of the collinear and/or massless limit. We present some examples of two-dimensional distributions for $F (Q_1^2,Q_2^2)$. A factorization breaking measure is proposed and factorization breaking effects are quantified and shown to be almost model independent. Factorization is shown to be strongly broken, and a scaling of the form factor as a function of $\bar Q^2 = (Q_1^2 + Q_2^2)/2$ is obtained.

Highlights

  • The description of the hadronic structure in terms of the quark and gluon degrees of freedom is one of the main goals of quantum chromodynamics (QCD)

  • For the light-front wave function (LFWF), we use different models obtained from the solution of the Schrödinger equation for a variety of ccpotentials

  • We compare our results to the BABAR experimental data for the ηcð1SÞ transition form factor, for one real and one virtual photon

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Summary

INTRODUCTION

The description of the hadronic structure in terms of the quark and gluon degrees of freedom is one of the main goals of quantum chromodynamics (QCD). A lot of attention has been paid to the case of pseudoscalar light meson-photon transition form factors [6,7], mainly motivated by the experimental data from the CLEO, BABAR, Belle, and L3 collaborations for the π0, η, and η0 production in eþe− collisions. These collaborations have extracted the transition form factor from single-tag events where only one of the leptons in the final state is measured.

Light-front wave function of ηc
Schrödinger equation and ccinteraction potentials
Light-front representation of the amplitude and transition form factor
NUMERICAL RESULTS
CONCLUSIONS
Full Text
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