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General Case

We are now left with the third case, where the electromagnetic radiation experiences both a different refractive index and a different extinction coefficient for its left and right circular polarizations while propagating in the material. As we have seen, different angular velocities means rotation of the linear polarization and different scattering/absorption means ellipticity. Consequently, the linearly polarized light in this case would exhibit both of these features and would follow a rotated ellipse, such as the one in figure 4.

 Fig. 4 Linearly polarized light as a combination of left (s - ) and right (s +  ) circularly polarized light in the case where the latter two experience different extinction coefficients  in the material and different phase velocities.

Ellipticity and rotation are then related by the Kronig-Kramers relations:

(Eq.4.1)

where P denotes the Cauchy Principal Value. The Kroning-Kramers transforms are a set of general mathematical equations that link the real and imaginary part of a complex number. They apply here since the optical rotation is related to the real part of the complex refractive index while ellipticity originates in its imaginary part. As you can see, it is possible to obtain the ellipticity at a given wavelength from a spectrum of optical rotation evaluations and vice-versa.

You now understand that any phenomenon that gives rise to a difference in the light-matter interaction for left and right circularly polarized light will result in an optical rotation and/or ellepticity. In the case of Circular Dichroism this is done because of chirality, while in the case of the Faraday effect, it originates in the magnetic field. We can then find that the Faraday rotation is given by:

(Eq.4.2)

where V is the Verdet constant, B the magnetic flux density and l is again the sample length. Identifying with Eq. 2.9 we see that the difference in refractive indices comes from the magnetic field. Exactly how much difference there is will depend on the material constant V, which also contains the wavelength information.


© V. K. Valev

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