Complex Structures in Electrodynamics
| dc.creator | Donev, Stoil | |
| dc.date | 2001-06-12 | |
| dc.date | 2001-11-02 | |
| dc.date.accessioned | 2026-07-07T04:28:30Z | |
| dc.date.available | 2026-07-07T04:28:30Z | |
| dc.description | In this paper we show that the basic external (i.e. not determined by the equations) object in Classical electrodynamics equations is a complex structure. In the 3-dimensional standard form of Maxwell equations this complex structure $\mathcal{I}$ participates implicitly in the equations and its presence is responsible for the so called duality invariance. We give a new form of the equations showing explicitly the participation of $\mathcal{I}$. In the 4-dimensional formulation the complex structure is extracted directly from the equations, it appears as a linear map $Φ$ in the space of 2-forms on $\mathbb{R}^4$. It is shown also that $Φ$ may appear through the equivariance properties of the new formulation of the theory. Further we show how this complex structure $Φ$ combines with the Poincare isomorphism $\mathfrak{P}$ between the 2-forms and 2-tensors to generate all well known and used in the theory (pseudo)metric constructions on $\mathbb{R}^4$, and to define the conformal symmetry properties. The equations of Extended Electrodynamics (EED) do not also need these pseudometrics as beforehand necessary structures. A new formulation of the EED equations in terms of a generalized Lie derivative is given. | |
| dc.description | Latex2e, 19 pages | |
| dc.identifier | https://arxiv.org/abs/math-ph/0106008 | |
| dc.identifier | http://arxiv.org/abs/math-ph/0106008 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/56811 | |
| dc.subject | Mathematical Physics | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | 78A02, 78A25, 78A97 | |
| dc.title | Complex Structures in Electrodynamics | |
| dc.type | text |