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We show that the geometric scaling of the dipole cross section can beexplained using standard DGLAP perturbative evolution. The DGLAP improvedsaturation model due to the Laplace transforms method is considered at LO andNNLO approximations from the experimental data by relying on aFroissart-bounded parametrization of $F_{2}(x,Q^{2})$. These results arecomparable with Golec-Biernat-W$\ddot{\mathrm{u}}$sthoff (GBW) model in a widekinematic region $rQ_{s}$ which takes into account charm mass. The successfuldescription of ${\sigma}_{\mathrm{dip}}(x,r)/\sigma_{0}$ and${\sigma}_{\mathrm{dip}}(rQ_{s})/\sigma_{0}$ are presented.

Color dipole cross section in the DGLAP improved saturation model