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Guided wave second-harmonic generation

Figure 5. Optimization of the cross-section for guided wave second harmonic generation. Phase-matching occurs between two dissimilar modes and the overlap integral is optimized by causing the interference effects to occur in linear regions of the waveguide only. For the case of a single nonlinear film, interference effects occur as the field product is integrated over the thickness dimension. Figure 5. Optimization of the cross-section for guided wave second harmonic generation. Phase-matching occurs between two dissimilar modes and the overlap integral is optimized by causing the interference effects to occur in linear regions of the waveguide only. For the case of a single nonlinear film, interference effects occur as the field product is integrated over the thickness dimension.
IV. PHASE MATCHING TECHNIQUES FOR GUIDED WAVE SECOND-HARMONIC GENERATION... [Pg.512]

See other pages where Guided wave second-harmonic generation is mentioned: [Pg.497]    [Pg.499]    [Pg.501]    [Pg.503]    [Pg.505]    [Pg.506]    [Pg.507]    [Pg.509]    [Pg.511]    [Pg.513]    [Pg.515]    [Pg.517]    [Pg.519]    [Pg.521]    [Pg.523]    [Pg.527]    [Pg.531]    [Pg.533]    [Pg.535]    [Pg.537]    [Pg.539]   


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