Download Anisotropic and Nonlinear Optical Waveguides by C.G. Someda and G.I. Stegeman (Eds.) PDF

By C.G. Someda and G.I. Stegeman (Eds.)

ISBN-10: 0444884890

ISBN-13: 9780444884893

Dielectric optical waveguides were investigated for greater than 20 years. within the final ten years they've got had the original place of being concurrently the spine of a truly useful and entirely constructed expertise, in addition to a very fascinating sector of easy, vanguard learn. current waveguides should be divided into units: one which include waveguides that are already in sensible use, and the Read more...

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Extra resources for Anisotropic and Nonlinear Optical Waveguides

Example text

7). 16), with Ν , is independently strongly of V, dependent the on summarized as follows: - in case a, grows proportionaly statistical V. Its 2 to N 1 ,/ and independently of the excitation-detection average behavior scheme this can of be happens (which, as we Random Birefringence and Polarization said before, influences the coefficients - in case b , grows as N r, where, the ratio between and scheme. 16)); r is close to 1; excitation-detection and < W > / N r is almost scheme; - in case c, grows linearly with N; the ratio between and Ν depends on the excitation-detection scheme.

001 (high correlation). 033 - as of F. G. 9) obtained with the Monte-Carlo simulation. 2b). The behaviors of (<Β>-σ β) and (<Β>+σ β) of are shown in fig. 5 for the three previous cases a, b and c. In case and c, the two curves which minimum expected represent values in practice for Β are the maximum practically indistinguishable from one another. Notice N ~ 1 ,/ 2while that for for uncorrelated strong fibers correlation it Β is is proportional proportional to to N" 1. The same conclusion applies to a smoothly varying fiber of length L, affected by random coupling and birefringence, characterized and aascorrelation if1 for L « Llength .

8 ) 56 R. Ddndliker Fo r V H Z = 0 on e find s A = ( A ) A, whic h confirm s reciprocit y (cf . 3 . L ) . e . i f th e twis t induce d circula r birefringenc e i s large r tha n th e expecte d linea r birefringenc e du e t o externa l perturbation s o f th e fiber, such as bendin g or squeezing . A silic a fiber wit h a diamete r of 2r = 8 0 ìô ç can b e subjecte d t o a torsio n of abou t Ô = 30÷2 ð rad/ m withou t risk of breaking , whic h yield s followin g Eq . 8 ) a twis t induce d circula r birefringenc e of ä = gT/ 2 = 1 5 rad/m .

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