Constraints in quantum mechanics

We discuss the introduction of constraints in a system of n noninteracting particles which obey the laws of nonrelativistic quantum mechanics. In this paper the particles are first thought of as being unconstrained (described by the $3n$ Cartesian coordinates of a flat space $R$), but subject to an external potential $V$ which, in a certian suitable limit, forces the system to remain in a curved subspace $V$ of $R$. This idea was already employed in a previous work where we have discussed the motion of one constrained particle. It was then shown that in order to obtain a meaningful result the particle wave function should be "uniformly compressed" into a surface (or curve), avoiding, in this way, the tangential forces which correspond to the dissipative constraints of classical mechanics. The resulting Schrödinger equation could then be separated in such a way that the part which contained the surface (or curve) variables was independent of the potential $V$ employed in the constraining process. In the present paper we show that this procedure cannot be carried out for all subspaces $V$ of $R$ in the case of a many-particle system, unless $V$ satisfies a certain geometrical condition. The many-particle Schrödinger equation (as was already the case of the one-particle systems) contains, besides the kinetic energy term, potentials which are not bending invariants, that is, cannot be obtained from the metric tensor $g_{\mathrm{ij}}$ of $V$ or its derivatives. This gives rise to different Schrödinger equations for isometric subspaces, in striking contrast with the usual quantization procedures which start from the classical Lagrangian of the constrained system.