Read e-book online Advances in Integrated Optics PDF

By S. Pelli, G. C. Righini (auth.), S. Martellucci, A. N. Chester, M. Bertolotti (eds.)

ISBN-10: 146136096X

ISBN-13: 9781461360964

ISBN-10: 1461525667

ISBN-13: 9781461525660

This volwne comprises the lawsuits of a two-week summer time convention titled "Advances in built-in Optics" held June 1-9, 1993, in Erice, Sicily. This was once the 18th annual direction prepared by means of the foreign college of Quantum Electronics, below the auspices of the "Ettore Majorana" Centre for medical tradition. The time period built-in Optics indicates guided-wave optical circuits along with or extra units on a unmarried substrate. on account that its inception within the overdue 1960's, built-in Optics has advanced from a really good study subject right into a large box of labor, starting from uncomplicated learn via advertisement functions. this present day many units can be found on marketplace whereas an enormous attempt is devolved to investigate on built-in nonlinear optical units. This convention was once equipped to supply a complete survey of the frontiers of this know-how, together with primary strategies, nonlinear optical fabrics, units either within the linear and nonlinear regimes, and chosen functions. those complaints replace and increase the fabric contained in a prior ISQE quantity, "Integrated Optics: Physics and Applications", S. Martellucci and A. N. Chester, Eds. , NATO ASI sequence B, Vol. ninety one (Plenum, 1983). For a few heavily similar expertise, the reader many additionally desire to seek advice the ISQE volumes: "Optical Fiber Sensors", A. N. Chester, S. Martellucci and A. M. Scheggi, Eds. , NATO ASI sequence E, Vol. 132 (Nijhoff, 1987) ; and, "Nonlinear Optics and Optical Computing", S. Martellucci and A. N. Chester, Eds. , E. Majorana Int'! technology sequence, Vol. forty nine (plenum, 1990).

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The variation of phase shift with z for kL = 4 and I a (w, 0) 12 = 25. 0 Fig. 30. The fractional fundamental intensity 1a (00, Z) 12/1 a (00. 0) 12 as a function of z for the same conditions as in Fig. 29. have shown that also in this case a nz coefficient can be defined which can either be positive (self-focusing) or negative (self-defocusing). The physical origin of this effective third order nonlinearity is straightforward. When the SHG process is mismatched, the second harmonic field propagates with the wavevector (55) Therefore the product E(2ro)E(ro)* in Eq.

Ostrowski, Electron. Lett. 28,139 (1992) 45. Mizuuchi. IEEE Photonics Techno\. Lett. 4, 435 (1992) 46. Watanabe, App!. Phys. Lett. 62,435 (1993) Nonlinear Guided Waves 53 47. L. J. J. Appl. Phys. 73,2695 (1993) 48. l. Pedersen, Appl. Opt. 31, 5813 (1992) 49. Wolf and W. Roc White, Opt. Lett. 17, 1779 (1992) 50. D. Bertolotti, and T. K. Tom, Opt. Lett. 17,396 (1992) 51. R. I. Stegeman, Opt. Lett. 4, 58 (1979) 52. R. I. Stegeman, Appl. Phys. Lett. 40, 759 (1982); R. I. Stegeman, Appl. Phys. Lett.

The angular dependence of the coupling efficiency with increasing incident cw power at J... 515 11m for a ZnS waveguide is shown. The excited nonlinearity was a thermal one. There is both a shift in the peak coupling angle and a decrease of efficiency, with a marked distortion of the curve with increasing power lO7 • Eventually bistability in the output versus input response is obtained (Fig. 16b). 2. Nonlinear Grating Coupling. In the case of grating coupling the resonant input coupling angle must satisfy the phase matching condition for the wave vectors of the input radiation 108 21t o - ko cos 80 + d m, (3(m) - (38) where (3~m) is the propagation constant of the guided wave, d is the grating period, ko =21t(A.

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Advances in Integrated Optics by S. Pelli, G. C. Righini (auth.), S. Martellucci, A. N. Chester, M. Bertolotti (eds.)


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