Optical Bit Error Rate

Chapter 2.9.3 - Birefringence

2.9.3   Birefringence

Anisotropic materials have a different index of refraction in specific directions. As
such, when a beam of monochromatic unpolarized light enters the material at a specific
angle and travels through it, it is refracted differently in the directions of different
indices (Figure 2.8). That is, when an unpolarized ray enters the material and
is separated into two rays, each with different polarization, different direction, and
different propagation constant; one is called the ordinary ray (O) and the other the
extraordinary ray (E). In these directions the refracted index is similarly called the
ordinary index, n0, and the extraordinary index, ne, respectively. This property of
crystals is known as birefringence. In general, all optically transparent crystals have
some degree of birefringence (some more than others), unless they belong to the cubic
system or they are amorphous.

Certain optically transparent isotropic materials become anisotropic when under
stress. Stress may be exerted due to mechanical forces (pulling, bending, twisting),
due to thermal forces (ambient temperature variations), and due to electrical fields.
Under such conditions, the index of refraction and polarization and propagation
characteristics become different in certain directions within the material.

Clearly, birefringence in fiber alters the polarization state of the characteristics
of the propagating optical signal, and several techniques have been developed to address
this phenomenon such as polarization spreading (polarization scrambling,
data-induced polarization), or polarization diversity.

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