Practical realization of perfect electromagnetic conductor (PEMC) boundaries using ferrites, magnet-less non-reciprocal metamaterials (MNMs) and graphene
2013 International Symposium on Electromagnetic Theory, 2013•ieeexplore.ieee.org
The perfect electromagnetic conductor (PEMC) was recently theoretically introduced by
Lindell and Sihvola as a fundamental hypothetical electromagnetic medium. This papers
proposes three related but distinct implementations-a ferrite, a magnet-less non-reciprocal
metamaterial (MNM) and a graphene implementation-of a practical PEMC boundary. These
implementations are all based on the combination of Faraday rotation and reflection from a
conductive ground, but exhibit distinct and complementary features.
Lindell and Sihvola as a fundamental hypothetical electromagnetic medium. This papers
proposes three related but distinct implementations-a ferrite, a magnet-less non-reciprocal
metamaterial (MNM) and a graphene implementation-of a practical PEMC boundary. These
implementations are all based on the combination of Faraday rotation and reflection from a
conductive ground, but exhibit distinct and complementary features.
The perfect electromagnetic conductor (PEMC) was recently theoretically introduced by Lindell and Sihvola as a fundamental hypothetical electromagnetic medium. This papers proposes three related but distinct implementations - a ferrite, a magnet-less non-reciprocal metamaterial (MNM) and a graphene implementation - of a practical PEMC boundary. These implementations are all based on the combination of Faraday rotation and reflection from a conductive ground, but exhibit distinct and complementary features.
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