The Effect of a Magnetic Flux Line in Quantum Theory
Abstract
The nonloclal exchange of the conserved, gauge invariant quantity ei (pk-ecAk)Lk, Lk=const., k=1,2 between the charged particle and the magnetic flux line (in the k=3 direction), is responsible for the Aharonov-Bohm effect. This exchange occurs at a definite time, before the wavepackets are brought together to interfere, and can be verified experimentally.
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