# Waves/Anisotropic Media

Waves : Geometrical Optics
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Problems

### Anisotropic MediaEdit

Notice that Snell's law makes the implicit assumption that rays of light move in the direction of the light's wave vector, i. e., normal to the wave fronts. As the analysis in the previous chapter makes clear, this is valid only when the optical medium is isotropic, i. e., the wave frequency depends only on the magnitude of the wave vector, not on its direction.

Certain kinds of crystals, such as those made of calcite, are not isotropic -- the speed of light in such crystals, and hence the wave frequency, depends on the orientation of the wave vector. As an example, the angular frequency in anisotropic medium might take the form

${\displaystyle \omega =\left[{\frac {c_{1}^{2}(k_{x}+k_{y})^{2}}{2}}+{\frac {c_{2}^{2}(k_{x}-k_{y})^{2}}{2}}\right]^{1/2},}$  (4.4)

where ${\displaystyle c_{1}}$  is the speed of light for waves in which ${\displaystyle k_{y}=k_{x}}$ , and ${\displaystyle c_{2}}$  is its speed when ${\displaystyle k_{y}=-k_{x}}$ .

Figure 3.3: The right panel shows the fate of a light ray normally incident on the face of a properly cut calcite crystal. The anisotropic dispersion relation which gives rise to this behavior is shown in the left panel.

Figure 3.3 shows an example in which a ray hits a calcite crystal oriented so that constant frequency contours are as specified in equation (3.4). The wave vector is oriented normal to the surface of the crystal, so that wave fronts are parallel to this surface. Upon entering the crystal, the wave front orientation must stay the same to preserve phase continuity at the surface. However, due to the anisotropy of the dispersion relation for light in the crystal, the ray direction changes as shown in the right panel. This behavior is clearly inconsistent with the usual version of Snell's law!

It is possible to extend Snell's law to the anisotropic case. We will not derive the equations here, but they are

${\displaystyle {\frac {dx_{i}}{dt}}={\frac {\partial \omega }{\partial k_{i}}}\quad {\frac {dk_{i}}{dt}}=-{\frac {\partial \omega }{\partial x_{i}}}}$

Later we will see a suggestive resemblance between these equation of geometrical optics and the equations of classical mechanics.

For now, though, we will assume that isotropic optical media are used, and discuss optical instruments.

Waves : Geometrical Optics
1 - 2 - 3 - 4 - 5 - 6
Problems