Abstract
Continuing the considerations given in the first part of this series (I), we use the analysis of the Aharonov-Bohm effect to show that the hydrodynamical variables by which the quantum mechanical one-body problem can be represented are of direct physical significance. It is shown in a particular case that the final state of a system can be obtained from its initial state in a unique manner if both states are characterized by hydrodynamical variables.
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References
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Jánossy, L. The physical interpretation of wave mechanics. II. Found Phys 4, 445–452 (1974). https://doi.org/10.1007/BF00708520
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DOI: https://doi.org/10.1007/BF00708520