The manifestly covariant Aharonov-Bohm effect in terms of the 4D fields
arXiv:1407.8459 · doi:10.1088/1742-6596/615/1/012015
Abstract
In this paper it is presented a manifestly covariant formulation of the Aharonov-Bohm (AB) phase difference for the magnetic AB effect . This covariant AB phase is written in terms of the Faraday 2-form F and using the decomposition of F in terms of the electric and magnetic fields as four-dimensional (4D) geometric quantities. It is shown that there is a static electric field outside a stationary solenoid with resistive conductor carrying steady current, which causes that the AB phase difference in the magnetic AB effect may be determined by the electric part of the covariant expression, i.e. by the local influence of the 4D electric field and not, as generally accepted,in terms of nonzero vector potential.
15 pages, sections 3 and 4 are enlarged and some new references are added,
References in corpus (9)
- On the role of potentials in the Aharonov-Bohm effect
- A macroscopic test of the Aharonov-Bohm effect
- The covariant, time-dependent Aharonov-Bohm Effect
- Comment on "Trouble with the Lorentz law of force: Incompatibility with special relativity and momentum conservation"
- Stokes' theorem, gauge symmetry and the time-dependent Aharonov-Bohm effect
- On the relation between the Feynman paradox and Aharonov-Bohm effects
- The 4D geometric quantities versus the usual 3D quantities. The resolution of Jackson's paradox
- Trouton-Noble paradox revisited
- The Lorentz transformations of the vectors E, B, P, M and the external electric fields from a stationary superconducting wire with a steady current and from a stationary permanent magnet