Abstract

The large-Q2Q^2 behavior of ηc\eta_c-γ\gamma and ηb\eta_b-γ\gamma transition form factors, Fηcγ(Q2)F_{\eta_c\gamma}(Q^2) and Fηbγ(Q2)F_{\eta_b\gamma}(Q^2) are analyzed in the framework of light-cone perturbative QCD with the heavy quark (cc and bb) mass effect, the parton's transverse momentum dependence and the higher helicity components in the light-cone wave function are respected. It is pointed out that the quark mass effect brings significant modifications to the asymptotic predictions of the transition form factors in a rather broad energy region, and this modification is much severer for Fηbγ(Q2)F_{\eta_b\gamma}(Q^2) than that for Fηcγ(Q2)F_{\eta_c\gamma}(Q^2) due to the bb-quark being heavier than the cc-quark. The parton's transverse momentum and the higher helicity components are another two factors which decrease the perturbative predictions. For the transition form factor Fηcγ(Q2)F_{\eta_c\gamma}(Q^2), they bring sizable corrections in the present experimentally accessible energy region (Q210GeV2Q^2 \leq 10 GeV^2). For the transition form factor Fηbγ(Q2)F_{\eta_b\gamma}(Q^2), the corrections coming from these two factors are negligible since the bb-quark mass is much larger than the parton's average transverse momentum. The coming e+ee^+ e^- collider (LEP2) will provide the opportunity to examine these theoretical predictions.Comment: 8 pages, RevTex, 5 PostScript figure

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