  In this paper we suggest a new approach to the structure of the soft Pomeron:
based on the $t$-channel unitarity, we expressed the exchange of the soft
Pomeron through the interaction of the dipole of small size of the order of
$1/Q_s(Y)$ ($Q_s(Y)$ is the saturation momentum) with the hadrons. Therefore,
it is shown that the typical distances in soft processes are small $r \sim
1/Q_s\Lb \h Y \Rb $, where $Y \,=\,ln s$. The saturation momentum, which
determines the energy dependence of the scattering amplitude is proportional to
$ Q^2_s\Lb \h Y \Rb \propto\,\exp\Lb\h \lambda\,Y\Rb$, with $\lambda
\approx\,0.2$, and this behaviour is in perfect agreement with phenomenological
Donnachie-Landshoff Pomeron. We demonstrate that the saturation models could
describe the experimental data for $\sigma_{tot},\sigma_{el},\sigma_{diff} $
and $B_{el}$. Hence our approach is a good first approximation to start
discussion of the soft processes in CGC approach on the solid theoretical
basis.
