Abstract

The notion of integrability in quantum mechanics is investigated in order to prepare rigorous grounds for the study of regular and irregular behaviour of quantum systems. Its common-sense definition turns out to have deficiencies which are illustrated by various explicit examples. Part of the ambiguities are shown to have their origin in the difficulty of transferring the concept of independent constants of motion into quantum mechanics, due to a fundamental theorem on sets of commuting operators by von Neumann. Taking into account the classical limit with coherent states does not resolve the problems. As a result, it is pointed out why the appealing phenomenological distinction between regular and chaotic quantum systems cannot be traced back to the present notion of “quantum integrability” in a mathematically rigorous way.

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