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Torrid

Introduction to Nonlinear Guided Wave Optics,sers, in the modern context semiconductor diode lasers with sub-watt powers can be used for observing many nonlinear phenomena. This development is the result of two factors, the most important being the development of better materials and the second the use of more optimum sample geometries. It is

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Second Order Nonlinear Optical Processes in KTiOPO4 Waveguides,and difference frequency generation, optical parametric generation and amplification, etc.[1] Most of these applications require very high input intensities to achieve reasonable conversion efficiencies and, hence, are mostly limited to use with high power laser or to resonant cavity systems.Confini

NEEDY

Organic Molecules for Guided Wave Quadratic and Cubic Optics,case of quadratic optics (electrooptic modulation,frequency doubling) the most promising at the present time are poled polymers with large second order nonlinear optical coefficients and good optical quality. With crosslinked polymers one obtains stable orientation over a long period of time..For cu

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LAPSE

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GaAs/GaAlAs Multiple Quantum Well Nonlinear Guided Wave Devices,ions is described for a range of different waveguide and quantum well geometries. It is shown that these nonlinearities are sufficiently strong to allow the realisation of all-optical switches for power levels in the range of lmW to 1μW. The recovery time to such switches is demonstrated to be in th

novelty

Third Order Nonlinear Integrated Optical Resonators,rpose, integrated optics offers major technological advantages such as: the concentration of light in waveguides, that is a requirement to combine speed and reasonable driving optical power,as well as the possibility to realize integrated optical circuits. Amidst all the integrated nonlinear optical

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