dc.contributor | 0000-0001-5324-1834 | |
dc.contributor | 0000-0002-1478-7946 | |
dc.creator | Chubykalo, Andrew | |
dc.creator | Espinoza, Augusto | |
dc.creator | Kosyakov, Boris Pavlovich | |
dc.date.accessioned | 2018-06-11T19:14:17Z | |
dc.date.accessioned | 2022-10-14T15:13:49Z | |
dc.date.available | 2018-06-11T19:14:17Z | |
dc.date.available | 2022-10-14T15:13:49Z | |
dc.date.created | 2018-06-11T19:14:17Z | |
dc.date.issued | 2011-12 | |
dc.identifier | 1286-4854 | |
dc.identifier | 0295-5075 | |
dc.identifier | http://hdl.handle.net/20.500.11845/523 | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/4247238 | |
dc.description.abstract | If the conventional Maxwell-Lorentz formulation of classical electrodynamics is
adopted in a flat spacetime of arbitrary odd dimension, then the retarded vector potential Aμ
generated by a point charge turns out to be pure gauge, Aμ = μ . By Gauss’ law, the charge
shows up as zero. The classical electromagnetic coupling is thus missing from odd-dimensional
worlds. If the action is augmented by the addition of the Chern-Simons term, then the classical
interaction picture in the three-dimensional world becomes nontrivial. | |
dc.language | eng | |
dc.publisher | The European Physical Society (EPS) | |
dc.relation | generalPublic | |
dc.relation | http://iopscience.iop.org/journal/0295-5075 | |
dc.rights | http://creativecommons.org/licenses/by-nc-sa/3.0/us/ | |
dc.rights | Atribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América | |
dc.source | EPL Journal, Núm. 96, Diciembre 2011. | |
dc.title | No-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worlds | |
dc.type | Artículos de revistas | |