The ratio ${\rho }_{\bar{p}p}^{pp}(s)$ in Froissaron and Maximal Odderon approach

The ratios ${\rho }_{\bar{p}p}^{pp}(s)$ of the real to the imaginary part of forward elastic $pp$ and $\bar{p}p$ scattering amplitudes at very high energies are considered in the models with rising total cross-sections and its difference. It is shown from the dispersion relations for $pp$ and $\bar{p}p$ scattering amplitudes that in the Froissaron and Maximal Odderon approach the ratios do not vanish asymptotically and they have the opposite signs for $pp$ and $\bar{p}p$ scattering.