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Non-linear crystals and frequency-mixing processes

In addition to the various tuneable laser sources described in the previous section, sources of tuneable [Pg.68]

only a short summary of the basic principles behind the non-linear effects is given, and some practical experimental realizations are discussed. [Pg.68]

All non-linear processes in crystalline materials rely on the fact that the macroscopic polarization of the medium, with non-linear susceptibility x, which is subjected to a strong electromagnetic field E, can be approximated as a power series expansion in terms of that applied field. The basic formalism for this, associated with the three-wave mixing processes of relevance here (i.e. two incident waves generate a new outgoing wave), is given in Box 4.1. [Pg.68]

In essence, the polarization induced in the nonlinear material by two incident waves E and Ei acts as a source of new waves at frequencies [Pg.68]

The new wave propagates through the non-linear medium with phase velocity [Pg.68]


See other pages where Non-linear crystals and frequency-mixing processes is mentioned: [Pg.68]    [Pg.69]    [Pg.71]   


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Crystal mixed crystals

Crystallization mixing

Crystallization processes

Crystallizer, mixed

Crystallizers mixing

Frequency-mixing processes

Linear frequency

Linear mixing

Mixed crystals

Mixing process linearization

Non mixing

Non-linear process

Non-linear processing

Process linear

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