Abstract
The quantum properties of localized finite energy solutions to classical Euler–Lagrange equations are investigated using the method of collective coordinates. The perturbation theory in terms of inverse powers of the coupling constant g is constructed, taking into account the conservation laws of momentum and angular momentum (invariance of the action with respect to the group of motion M(3) of three-dimensional Euclidean space) rigorously in every order of perturbation theory.
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