Abstract
In Chapter 2, where the electromagnetic theory of light was briefly described, the basic properties of the propagation of a light ray in a crystal were studied. It was shown that when a light ray enters a crystal, it splits into two rays that are linearly polarized at right angles to each other, which propagate with different velocities. The refractive index associated with each light ray in the crystal can be found by use of Fresnel’s ellipsoid, which shows, for any point in the crystal, the variation of refractive index with direction of the light ray. This splitting of rays into two rays that have mutually perpendicular polarizations results from a physical property of crystalline materials that is called optical birefringence or simply birefringence.
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Theocaris, P.S., Gdoutos, E.E. (1979). The Photoelastic Phenomenon. In: Matrix Theory of Photoelasticity. Springer Series in Optical Sciences, vol 11. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-35789-6_6
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