The ργ∗→π(ρ)ργ^* \to π(ρ) transition form factors in the Perturbative QCD factorization approach

preprint2015arXivOpen access

Abstract

In this paper, we studied the ργ∗→πργ^* \to π and ργ∗→ρργ^*\to ρ transition processes and made the calculations for the ρπρπ transition form factor Q4Fρπ(Q2)Q^4 F_{ρπ}(Q^2) and the ρρ meson electromagnetic form factors, FLL,LT,TT(Q2)F_{\rm LL, LT,TT}(Q^2) and F1,2,3(Q2)F_{1,2,3}(Q^2), by employing the perturbative QCD (PQCD) factorization approach. For the ργ∗→πργ^* \to π transition, we found that the contribution to form factor Q4Fρπ(Q)Q^4 F_{ρπ}(Q) from the term proportional to the distribution amplitude combination ϕρT(x1)ϕπP(x2)ϕ^T_ρ(x_1)ϕ^P_π(x_2) is absolutely dominant, and the PQCD predictions for both the size and the Q2Q^2-dependence of this form factor Q4Fρπ(Q2)Q^4 F_{ρπ}(Q^2) agree well with those from the extended ADS/QCD models or the light-cone QCD sum rule. For the ργ∗→ρργ^* \to ρ transition and in the region of Q2≥3Q^2\geq 3 GeV2^2, further more, we found that the PQCD predictions for the magnitude and their Q2Q^2-dependence of the F1(Q2)F_1(Q^2) and F2(Q2)F_2(Q^2) form factors agree well with those from the QCD sum rule, while the PQCD prediction for F3(Q2)F_3(Q^2) is much larger than the one from the QCD sum rule.

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