3 - General properties of the optical constants

Summary

In Chapter 2 we described the propagation of electromagnetic radiation in free space and in a homogeneous medium, together with the changes in the amplitude and phase of the fields which occur at the interface between two media. Our next objective is to discuss some general properties of what we call the response of the medium to electromagnetic fields, properties which are independent of the particular description of solids; i.e. properties which are valid for basically all materials. The difference between longitudinal and transverse responses will be discussed first, followed by the derivation of the Kramers–Kronig relations and their consequences, the so-called sum rules. These relations and sum rules are derived on general theoretical grounds; they are extremely useful and widely utilized in the analysis of experimental results.

Longitudinal and transverse responses

General considerations

The electric field strength of the propagating electromagnetic radiation can be split into a longitudinal component E^L=(n_q·E)n_q and a transverse component E^T=(n_q×E)×n_q, with E=E^L+E^T, where n_q=q/|q| indicates the unit vector along the direction of propagation q. While E^L∥q, the transverse part E^T lies in the plane perpendicular to the direction q in which the electromagnetic radiation propagates; it can be further decomposed into two polarizations which are usually chosen to be normal to each other.