Can the permittivity tensor always be diagonalized?
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For an anisotropic medium, permittivity is a symmetric tensor, with elements as ϵijϵij
How can one be sure that it is diagonalizable, if some elements, say ϵxyϵxy and ϵyxϵyx are imaginary
How can one be sure that it is diagonalizable, if some elements, say ϵxyϵxy and ϵyxϵyx are imaginary
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Clearly, then, one cannot locally diagonalize the metric tensor in general (or else every Riemann manifold would be locally isometric to some Euclidean space.
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