The normal state of the Holstein model is studied at half-filling in infini
te dimensions and in the adiabatic regime. The dynamical mean-field equatio
ns are solved using perturbation expansions around the extremal paths of th
e effective action for the atoms. We find that the Migdal-Eliashberg expans
ion breaks dawn in the metallic state if the electron-phonon coupling lambd
a exceeds a value of about 1.3 in spite of the fact that the formal expansi
on parameter lambda omega(0)/E-F (omega(0) is the phonon frequency, E-F the
Fermi energy) is much smaller than 1. The breakdown is due to the appearan
ce of more than one extremal path of the action. We present numerical resul
ts which illustrate in detail the evolution of the local Green's function,
the self-energy, and the effective atomic potential as a function of lambda
. [S0163-1829(98)01845-1].