2012
DOI: 10.1016/j.aop.2011.09.005
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Covariant jump conditions in electromagnetism

Abstract: A generally covariant four-dimensional representation of Maxwell's electrodynamics in a generic material medium can be achieved straightforwardly in the metric-free formulation of electromagnetism. In this setup, the electromagnetic phenomena described by two tensor fields, which satisfy Maxwell's equations. A generic tensorial constitutive relation between these fields is an independent ingredient of the theory. By use of different constitutive relations (local and non-local, linear and non-linear, etc.), a w… Show more

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Cited by 7 publications
(8 citation statements)
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References 27 publications
(49 reference statements)
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“…Once more we have two optic axes. 4) In the last case, 42) there is only one eigenvalue m = 0 of multiplicity four. It corresponds to two eigenvectors q = (β, 0, 0, ±α), and consequently there are again two optic axes.…”
Section: Proofmentioning
confidence: 99%
See 3 more Smart Citations
“…Once more we have two optic axes. 4) In the last case, 42) there is only one eigenvalue m = 0 of multiplicity four. It corresponds to two eigenvectors q = (β, 0, 0, ±α), and consequently there are again two optic axes.…”
Section: Proofmentioning
confidence: 99%
“…The covariant boundary surface problem was studied in [31] and [42]. In particular, when the space-time decomposition of the fields F and H is applied and the fields are assumed to be independent of the time coordinate, Eqs.…”
Section: B Covariant Jump Conditions and Wavefrontmentioning
confidence: 99%
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“…Symbol and hyperbolic polynomials of the wave equation and their relation to premetric electrodynamics were discussed by Beig [5]. Itin [35] derived premetric covariant jump conditions for the initial value hypersurface, the light cone, and a boundary between two media.…”
mentioning
confidence: 99%