The Quantum Stationary HJ Equation (QSHJE) that we derived from the equival
ence principle, gives rise to initial conditions which cannot be seen in th
e Schrodinger equation. Existence of the classical limit leads to a depende
nce of the integration constant l = l(1) + il(2) on the Planck length. Solu
tions of the QSHJE provide a trajectory representation of quantum mechanics
which, unlike Bohm's theory, has a non-trivial action even for bound state
s and no wave guide is present. The quantum potential turns out to be an in
trinsic potential energy of the particle which, similarly to the relativist
ic rest energy, is never vanishing. (C) 1998 Elsevier Science B.V. All righ
ts reserved.