  In this paper, through an exhaustive analysis within the Migdal-Eliashberg
theory, we show the incompatibility of experimental data of Rb$_3$C$_{60}$ with
the basic assumptions of the standard theory of superconductivity. For
different models of the electron-phonon spectral function $\alpha^2F(\Omega)$
we solve numerically the Eliashberg equations to find which values of the
electron-phonon coupling $\lambda$, of the logarithmic phonon frequency
$\Omega_{ln}$ and of the Coulomb pseudopotential $\mu^*$ reproduce the
experimental data of Rb$_3$C$_{60}$. We find that the solutions are essentially
independent of the particular shape of $\alpha^2F(\Omega)$ and that, to explain
the experimental data of Rb$_3$C$_{60}$, one has to resort to extremely large
couplings: $\lambda=3.0\pm 0.8$. This results differs from the usual partial
analyses reported up to now and we claim that this value exceeds the maximum
allowed $\lambda$ compatible with the crystal lattice stability. Moreover, we
show quantitatively that the obtained values of $\lambda$ and $\Omega_{ln}$
strongly violate Migdal's theorem and consequently are incompatible with the
Migdal-Eliashberg theory. One has therefore to consider the generalization of
the theory of superconductivity in the nonadiabatic regime to account for the
experimental properties of fullerides.
