A magnetooptic effect is any one of a number of phenomena in which an electromagnetic wave propagates through a medium that has been altered by the presence of a quasistatic magnetic field. In such a material, which is also called gyrotropic or gyromagnetic, left and rightrotating elliptical polarizations can propagate at different speeds, leading to a number of important phenomena. When light is transmitted through a layer of magnetooptic material, the result is called the Faraday effect: the plane of polarization can be rotated, forming a Faraday rotator. The results of reflection from a magnetooptic material are known as the magnetooptic Kerr effect (not to be confused with the nonlinear Kerr effect).
In general, magnetooptic effects break time reversal symmetry locally (i.e. when only the propagation of light, and not the source of the magnetic field, is considered) as well as Lorentz reciprocity, which is a necessary condition to construct devices such as optical isolators (through which light passes in one direction but not the other). (The other, less useful, way to break time reversal symmetry is to rely upon absorption loss.)
Two gyrotropic materials with reversed rotation directions of the two principal polarizations, corresponding to complexconjugate ε tensors for lossless media, are called optical isomers.
Gyrotropic permittivity
In particular, in a magnetooptic material the presence of a magnetic field (either externally applied or because the material itself is ferromagnetic) can cause a change in the permittivity tensor ε of the material. The ε becomes anisotropic, a 3×3 matrix, with complex offdiagonal components, depending of course on the frequency ω of incident light. If the absorption losses can be neglected, ε is a Hermitian matrix. The resulting principal axes become complex as well, corresponding to ellipticallypolarized light where left and rightrotating polarizations can travel at different speeds (analogous to birefringence).
More specifically, for the case where absorption losses can be neglected, the most general form of Hermitian ε is:
or equivalently the relationship between the displacement field D and the electric field E is:
where is a real symmetric matrix and is a real pseudovector called the gyration vector, whose magnitude is generally small compared to the eigenvalues of . The direction of g is called the axis of gyration of the material. To first order, g is proportional to the applied magnetic field:
where is the magnetooptical susceptibility (a scalar in isotropic media, but more generally a tensor). If this susceptibility itself depends upon the electric field, one can obtain a nonlinear optical effect of magnetooptical parametric generation (somewhat analogous to a Pockels effect whose strength is controlled by the applied magnetic field).
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