Abstract

We study the $e^+e^-\to VP$ and $e^+e^-\to TP$ processes in the perturbative QCD approach based on $k_T$ factorization, where the $P,V$ and $T$ denotes a light pseudo-scalar, vector and tensor meson, respectively. We point out in the case of $e^+e^-\to TP$ transition due to charge conjugation invariance, only three channels are allowed: $e^+e^-\to a_2^{\pm} \pi^\mp$, $e^+e^-\to K_2^{*\pm} K^\mp$ and the V-spin suppressed $e^+e^-\to K_2^{*0} \bar K^0+\overline K_2^{*0} K^0 $. Cross sections of $e^+e^-\to VP$ and $e^+e^-\to TP$ at $\sqrt{s}=3.67$ GeV and $\sqrt{s}=10.58$ GeV are calculated and the invariant mass dependence is found to favor the $1/s^4$ power law. Most of our theoretical results are consistent with the available experimental data and other predictions can be tested at the ongoing BESIII and forthcoming Belle-II experiments.

Highlights

  • The exclusive processes of eþe− annihilating into two mesons provide an opportunity to investigate various timelike meson form fpacffiffitors

  • We study the eþe− → VP and eþe− → TP processes in the perturbative QCD approach based on kT

  • A modified perturbative QCD approach based on kT factorization, called PQCD approach for brevity, is proposed [6,7,8,9,10,11] and has been successfully applied to many reactions [5,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27]

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Summary

INTRODUCTION

The exclusive processes of eþe− annihilating into two mesons provide an opportunity to investigate various timelike meson form fpacffiffitors. It is anticipated that hard exclusive processes with hadrons involve both perturbative and nonperturbative strong interactions. A modified perturbative QCD approach based on kT factorization, called PQCD approach for brevity, is proposed [6,7,8,9,10,11] and has been successfully applied to many reactions [5,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27] In this approach, the transverse momentum of partons in the meson is kept to kill endpoint divergences.

Notations
Decay constants and light cone wave functions
PQCD calculation
NUMERICAL RESULTS AND DISCUSSIONS
CONCLUSION
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