|
| related topics |
| {field, particle, equation} |
| {wave, scattering, interference} |
| {time, wave, function} |
| {phase, path, phys} |
| {cos, sin, state} |
| {measurement, state, measurements} |
| {operator, operators, space} |
|
The Effect of a Magnetic Flux Line in Quantum Theory
Y. Aharonov, T. Kaufherr
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.
- oai_identifier:
- oai:arXiv.org:quant-ph/0402203
- categories:
- quant-ph
- comments:
- LaTeX, 13 pages with 3 figures
- doi:
- 10.1103/PhysRevLett.92.070404
- arxiv_id:
- quant-ph/0402203
- journal_ref:
- Physical Review Letters 92, 7, 070404 (2004)
- report_no:
- TAUP 2674-2001
- created:
- 2004-02-26
Full article ▸
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