  We revisit the rapidity dependence of the average transverse momentum
$\left\langle p_{T}\right\rangle$ in a $pp$ and $pA$ collision, using the high
energy factorization (HEF). We update previous predictions for the
$\left\langle p_{T}\right\rangle$ both in central and forward rapidity region
using parton densities following from extended BK and BFKL evolution equations
to account for corrections of higher orders as well as one obtained by Sudakov
resummation. Furthermore, we demonstrate that in the mid rapidity region the
saturation based formalisms predict increase of the transversal momentum while
in the forward rapidity region the $\left\langle p_{T}(y)\right\rangle$
decreases.
