Abstract

We obtain the distribution amplitude (DA) of the pion from its light-front wave functions in the basis light-front quantization framework. This light-front wave function of the pion is given by the lowest eigenvector of a light-front effective Hamiltonian consisting a three-dimensional confinement potential and the color-singlet Nambu--Jona-Lasinion interaction both between the constituent quark and antiquark. The quantum chromodynamics (QCD) evolution of the DA is subsequently given by the perturbative Efremov-Radyushkin-Brodsky-Lepage evolution equation. Based on this DA, we then evaluate the singly and doubly virtual transition form factors in the space-like region for $\pi^0\rightarrow \gamma^*\gamma$ and $\pi^0\rightarrow \gamma^*\gamma^*$ processes using the hard-scattering formalism. Our prediction for the pion-photon transition form factor agrees well with data reported by the Belle Collaboration. However, in the large $Q^2$ region it deviates from the rapid growth reported by the BaBar Collaboration. Meanwhile, our result on the $\pi^0\rightarrow \gamma^*\gamma^*$ transition form factor is also consistent with other theoretical approaches and agrees with the scaling behavior predicted by perturbative QCD.

Highlights

  • The parton distribution amplitudes (DAs) that play essential roles in describing the various hard exclusive processes of quantum chromodynamics (QCD) bound states [1–3] via the factorization theorem [4] are among the most basic structure functions

  • We have evaluated the valence-quark distribution amplitude from the light-front wave functions (LFWFs) of the pion in the framework of the basis light front quantization (BLFQ)

  • Our result is based on the wave functions as the eigenfunctions of an effective Hamiltonian which includes the confinement potentials and the color-singlet NambuJona-Lasinio interactions

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Summary

INTRODUCTION

The parton distribution amplitudes (DAs) that play essential roles in describing the various hard exclusive processes of quantum chromodynamics (QCD) bound states [1–3] via the factorization theorem [4] are among the most basic structure functions. [1,29], where TFFs are expected to follow the asymptotic behavior of, Q2FPγðQ2Þ → constant as Q2 → ∞ Unlike their results showing growth in Q2FπγðQ2Þ, the BABAR data [28] for the Q2Fðη;η0ÞγðQ2Þ appear consistent with the PQCD. The meson (M) TFFs for the doubly virtual M → γÃγà transitions have been studied within the Dyson-Schwinger and Bethe-Salpeter framework [52], the chiral perturbation theory [53], a light-front quark model [54], the anti–de Sitter (AdS)/QCD [55,56], and the lattice QCD [16,57–60]. The nonperturbative solutions for the LFWFs given by the recent BLFQ study of light mesons [67] have been applied successfully to predict the electromagnetic form factors and associated charge radii, PDFs, structure functions and generalized parton distributions of the pion [67–70]. We extend our investigations of the pion to compute its singly and doubly virtual photon TFFs

BLFQ-NJL MODEL FOR THE LIGHT MESONS
PARTON DISTRIBUTION AMPLITUDE
PION TO PHOTONS TRANSITION FORM FACTORS
SUMMARY
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