The Effect of a Magnetic Flux Line in Quantum Theory
| dc.creator | Aharonov, Y. | |
| dc.creator | Kaufherr, T. | |
| dc.date | 2004-02-26 | |
| dc.date.accessioned | 2026-07-07T06:09:09Z | |
| dc.date.available | 2026-07-07T06:09:09Z | |
| dc.description | 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. | |
| dc.description | LaTeX, 13 pages with 3 figures | |
| dc.identifier | https://arxiv.org/abs/quant-ph/0402203 | |
| dc.identifier | http://arxiv.org/abs/quant-ph/0402203 | |
| dc.identifier | Physical Review Letters 92, 7, 070404 (2004) | |
| dc.identifier | doi:10.1103/PhysRevLett.92.070404 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/91866 | |
| dc.subject | Quantum Physics | |
| dc.title | The Effect of a Magnetic Flux Line in Quantum Theory | |
| dc.type | text |