  In this paper, we use the re-summation procedure, suggested in
Refs.\cite{DIMST,SALAM,SALAM1,SALAM2}, to fix the BFKL kernel in the NLO.
However, we suggest a different way to introduce th non-linear corrections in
the saturation region, which is based on the leading twist non-linear equation.
In the kinematic region:$\tau\,\equiv\,r^2 Q^2_s(Y)\,\leq\,1$ , where $r$
denotes the size of the dipole, $Y$ its rapidity and $Q_s$ the saturation
scale, we found that the re-summation contributes mostly to the leading twist
of the BFKL equation. Assuming that the scattering amplitude is small, we
suggest using the linear evolution equation in this region. For $\tau \,>\,1$
we are dealing with the re-summation of $\Lb \bas \,\ln \tau\Rb^n$ and other
corrections in NLO approximation for the leading twist.We find the BFKL kernel
in this kinematic region and write the non-linear equation, which we solve
analytically. We believe the new equation could be a basis for a consistent
phenomenology based on the CGC approach.
