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The Effect of a Magnetic Flux Line in Quantum Theory

Y. Aharonov·T. Kaufherr
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Abstract

The nonloclal exchange of the conserved, gauge invariant quantity $e^{\frac{i}{\hbar} (p_{k}-\frac{e}{c}A_{k})L^{k}}, L^{k}=const., k=1,2$ 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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BibTeXRIS

Y. Aharonov, T. Kaufherr. 2004-02-26. The Effect of a Magnetic Flux Line in Quantum Theory. https://doi.org/10.1103/physrevlett.92.070404

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