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2.7 Classification of Bianisotropic Media

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It is sometimes convenient to classify bianisotropic media in terms of their tensorial constitutive parameters. For this purpose, we split the susceptibility tensors and into a tensor, , related to nonreciprocity, and a tensor, , related to chirality [148], as

(2.85)

Table 2.3 classifies the reciprocal ( and ) and nonreciprocal ( and ) bianisotropic media depending on whether the tensors or are diagonal or not, and symmetric or antisymmetric, respectively. This classification relies on the fact that an arbitrary tensor , which may represent either (for a reciprocal medium) or (for a nonreciprocal medium), can be decomposed as

(2.86)

Table 2.3 Classification of bianisotropic media [148].

Type Parameters Medium
Reciprocal Omega
Pseudochiral
Pseudochiral omega
Pasteur (or biisotropic)
Chiral omega
Anisotropic chiral
General reciprocal
Nonreciprocal Moving
Pseudo Tellegen
Moving pseudo Tellegen
Tellegen
Moving Tellegen
Anisotropic Tellegen
Nonreciprocal nonchiral

where is a diagonal tensor and is a traceless tensor that can be further split into a symmetric part, , and an antisymmetric part, , where

(2.87)

such that (2.86) becomes

(2.88)

Electromagnetic Metasurfaces

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