By Christos Flytzanis (auth.), A. Miller, K. R. Welford, B. Daino (eds.)

Nonlinear Optical fabrics and units for functions in details Technology takes the reader from basic interactions of laser mild in fabrics to the newest advancements of electronic optical info processing. The e-book emphasises nonlinear optical interactions in bulk and low-dimensional semiconductors, liquid crystals and optical fibres. After developing the fundamental laser--material interactions in those fabrics, it is going directly to examine purposes in soliton propagation, built-in optics, clever pixel arrays and electronic optical computing.

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Extra info for Nonlinear Optical Materials and Devices for Applications in Information Technology

Sample text

It is evident from the above qualitative discussion that for most purposes in nonlinear optics one may start by setting up the expression of the induced polarization in the dipole approximation. We will restrict ourselves in the most commonly recurring case where the material is composed of identical repeat polarizable entities, atoms, molecules or clusters of dimensions much smaller than the optical wavelength ; these will be either randomly but homogeneously distributed, like for instance in a gas, a liquid or an amorphous solid or set in a periodic array, for instance a crystalline solid.

The quadru-polarization and the magnetic polarization in (55) result from such considerations. Their inclusion in the Maxwell equations opens up a whole class of phenomena which besides the natural spatial dispersion and optical activity (gyrotropy) also includes artificial gyrotropy (Faraday rotation), Cotton-Mouton effects but also the photoinduced ones and others. Because of their different nature with respect to the dipolar ones we shall not dwell further upon these effects here except to point out that in the near future a growing attention and studies will be focused on them with important implications in a number of applications.

One finds that here the refractive indices for right and left circular polarization become different and these two components experience different phase shifts after propagating a distance L inside the medium ; the polarization state undergoes a rotation by an angle 8p = roL nc (n · - n+ ) (47) 27 the Faraday rotation angle. In tenns of susceptibilities we also have where~ X~1 ) is the static magnetic field induced change of the linear susceptibility x and can be related to X~) (co,O) in (46).

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