| dc.creator | | |
| dc.creator | | |
| dc.creator | Andrew Chubykalo | |
| dc.creator | | |
| dc.date | 2011-12 | |
| dc.date.accessioned | 2022-10-12T19:49:22Z | |
| dc.date.available | 2022-10-12T19:49:22Z | |
| 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/2250/4122767 | |
| dc.description | 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.description | Producción Científica de la Universidad Autónoma de Zacatecas UAZ | |
| dc.format | application/pdf | |
| dc.language | eng | |
| dc.rights | info:eu-repo/semantics/openAccess | |
| dc.rights | http://creativecommons.org/licenses/by-nc-nd/4.0 | |
| dc.subject | info:eu-repo/classification/cti/1 | |
| dc.subject | Classical electromagnetism | |
| dc.subject | Maxwell equations | |
| dc.subject | Field theories in dimensions other than four | |
| dc.title | No-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worlds | |
| dc.type | info:eu-repo/semantics/article | |
| dc.audience | generalPublic | |
