No-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worlds

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Published 30 November 2011 Europhysics Letters Association
, , Citation A. E. Chubykalo et al 2011 EPL 96 60001 DOI 10.1209/0295-5075/96/60001

0295-5075/96/6/60001

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=∂μχ. 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.

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10.1209/0295-5075/96/60001