Hamiltonian equations are formulated in terms of collective variables descr
ibing the dynamics of the soliton of an integrable nonlinear Schrodinger eq
uation on a 1D lattice. Earlier, similar equations of motion were suggested
for the soliton of the nonlinear Schrodinger equation in partial derivativ
es. The operator of soliton momentum in a discrete chain is defined; this o
perator is unambiguously related to the velocity of the center of gravity o
f the soliton. The resulting Hamiltonian equations are similar to those for
the continuous nonlinear Schrodinger equation, but the role of the field m
omentum is played by the summed quasi-momentum of virtual elementary system
excitations related to the soliton. (C) 2001 MAIK "Nauka/Interperiodica".