  In this article, we calculate the axial and the induced pseudoscalar
form-factors $G_A(t=-Q^2)$ and $G_P(t=-Q^2)$ of the nucleons in the framework
of the light-cone QCD sum-rules approach up to twist-6 three valence quark
light-cone distribution amplitudes, and observe that the form-factors
$G_A(t=-Q^2)$ and $G_P(t=-Q^2)$ at intermediate and large momentum transfers
with $Q^2> 2 GeV^2$ have significant contributions from the end-point (soft)
terms. The numerical values for the axial form-factor $G_A(t=-Q^2)$ are
compatible with the experimental data and theoretical calculations, for
example, the chiral quark models and lattice QCD. The numerical values for the
induced pseudoscalar form-factor $G_P(t=-Q^2)$ are compatible with the
calculation from the Bethe-Salpeter equation.
