The Crystallization of polarons at finite density, due to the long-range Co
ulomb forces - when no bipolarons can be formed - is discussed close to the
metal-insulator transition (MIT). As a function of the density, the meltin
g is examined at zero temperature. By calculating the quantum fluctuations
of both the electron and the polarization, we show that at strong electron-
phonon coupling the dissociation of the polarons at the MIT is favored, rat
her than the melting towards a polaron liquid. In this regime, we demonstra
te that an instability of the transverse vibrational modes of the polaron c
rystal occurs as the density increases. This provides a new physical mechan
ism for the MIT in polar materials, for which an experimental signature is
predicted.