Abstract
The explicit forms of the broken (by a electric field E, magnetic field H and spatial dispersion of wave vector k) point symmetry groups of a crystal are given. For these groups the dielectric permeability tensors: eij (ω, E), eij (ω, H) and ei j (ω, k) — the particular cases of eij (ω, E, H, k) — are written out (the susceptibility tensors x,, (ω, E), χij (ω, H) and χij (ω, k) take the same forms). In order to illustrate the results obtained the electrooptical phenomena (connected with the tensors (ω, E)) are discussed.
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