Depending on the context, Hadronic Form Factors and DECAY constants are equivalent concepts, where a decay constant for some pseudoscalar meson M:
<br />
\langle 0| q_1 \gamma^\mu (1-\gamma_5) q_2 | M > = -i f_M p^{\mu}_{M}<br />
is part of the parametrization of the matrix, in this case a constant, but say for a vector meson decay
<br />
\langle \gamma | q_1 \gamma^\mu (1-\gamma_5) q_2 | V > = F_V (q^2) \epsilon^{\mu \nu \alpha \beta} \eta^\nu p_{V\alpha} p_{\gamma \beta} + i F_A (q^2) [\eta^\mu (p_V \cdot p_\gamma ) - p^{\gamma \mu} (p_V \cdot \eta)]<br />
Where Fv and Fa are the form factors of the parametrization of this decay. Similar ideas but the "scalars" in the second case are functions of the momentum transfer, while in the first must not depend on momentum, as there is no transfer.
Maybe that's what you meant?