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Direct Energy, 2018a

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56 3.3 Electro-Optics<br />

KH 2 PO 4 [25] [26]. It has also been studied in chalcogenide glasses which are<br />

suldes, selenides, and tellurides such as GeTe [25] [26]. When selecting a<br />

pyroelectric material for an application, the pyroelectric coecient should<br />

be considered. Thermal properties are important too. The material should<br />

be able to withstand repeated heating and cooling, and it should have a<br />

relatively high melting temperature to be useful.<br />

The pyroelectric eect does not have many applications. Some optical<br />

detectors designed to detect infrared light are made from pyroelectric materials<br />

[41] [42]. However, most optical detectors are photovoltaic devices<br />

made from semiconductor junctions, and this technology will be discussed<br />

in Chapter 6. While sensors using the pyroelectric eect could be used to<br />

measure temperature, other types of temperature sensors, such as thermocouples,<br />

are typically used. Thermocouples, which operate based on the<br />

thermoelectric eect which is discussed in Chapter 8, are more convenient<br />

to build and operate. Additionally, in many pyroelectric materials, the effect<br />

is nonlinear while linear sensors are easier to work with and calibrate.<br />

3.3 Electro-Optics<br />

3.3.1 Electro-Optic Coecients<br />

Typically, the magnitude of material polarization in a dielectric is proportional<br />

to the strength of an applied electric eld.<br />

−→ −→ −→ −→ P = D − ɛ0 E = ɛ0 χ e E (3.3)<br />

In this equation χ e is the electric susceptibility, and it is unitless. It is<br />

dened in Sec. 2.2.3 and related to permittivity by Eq. 2.9. However in<br />

other materials, the material polarization depends nonlinearly on the applied<br />

electric eld. Materials for which the material polarization depends<br />

linearly on the external electric eld are called linear materials while others<br />

are called nonlinear or electro-optic materials. The electro-optic eect occurs<br />

when an applied external electric eld induces a material polarization<br />

in a material where the amount of polarization depends nonlinearly on the<br />

external eld. The name involves the word optic because the external eld<br />

is often due to a visible laser beam. However, the external eld can be<br />

from any type of source at any frequency, and a material polarization will<br />

occur even with a constant applied electric eld. A large enough external<br />

electric eld will cause a material to melt or to crystallize in a dierent<br />

phase, but this eect is not the electro-optic eect. Instead, the electrooptic<br />

eect only involves a change in the material polarization, not the<br />

crystal structure, and the change involved is not permanent.

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