We analyze the phase transition of a strictly two-dimensional electron
crystal (Wigner lattice) to an electron liquid, at zero temperature.
The phase transition is discussed in a model based on the interaction
of a dislocated electron with phonons of a regular Wigner lattice. Wit
h the careful treatment of polaron self-energy, this theory gives the
electron melting density in very good agreement with the result obtain
ed from the first-principle calculations of Tanatar and Ceperley.