  Froissart Bound implies that the total proton-proton cross-section (or
equivalently structure function) cannot rise faster than the logarithmic growth
$\log^2 s \sim \log^2 (1/x)$, where \textit{s} is the square of the center of
mass energy and \textit{x} is the Bjorken variable. In the present report,
compatibility of such behavior will be shown in case of Transverse Momentum
Dependent Parton Distributions Functions (TMDPDF) or TMDs for the model of
proton based on self-similarity.
