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5) and therefore can be interpreted by the zig-zag wave model. The left-hand 8 Waveguides, Optical side of Eq. (39) represents the phase acquired by the zigzag wave in the guiding region (0 < x < xt ). The right-hand side implies that the wave acquires a (half) phase shift of −π/4 at the turning point, where total internal reflection takes place, and a (half) phase shift of − at the surface. The phase shift in Eq. (39) is in fact identical to the phase shift 3 given by Eq. (6). Under the condition n21 − n22 n21 − n23 , it follows that 3 ∼ = π2, regardless of the polarization of the wave.

8 (5): 644–646, 1996. 30. M. , 33-GHz-cm broadband Ti:LiNbO3 Mach-Zehnder modulator, ECOC Tech. , 1989, Paper ThB22-5. 31. G. K. , Performance and modeling of broadband LiNbO3 traveling wave optical intensity modulators, J. Lightw. , 12 (10): 1807–1819, 1994. 32. K. Kawano, High-speed shielded velocity-matched Ti:LiNbO3 optical modulator, IEEE J. , QE-29 (9): 2466– 2475, 1993. 33. K. Noguchi, O. Mitomi, and H. Miyazawa, Low-voltage and broadband Ti:LiNbO3 modulators operating in the millimeter wavelength region, Proc.

See INTEGRATED OPTOELECTRONICS. htm }{{}} ● HOME ● ABOUT US ● CONTACT US ● HELP Home / Engineering / Electrical and Electronics Engineering Wiley Encyclopedia of Electrical and Electronics Engineering Integrated Optic Waveguides Standard Article Kin Seng Chiang1 1Department of Electronic Engineering, City University of Hong Kong, Kowloon, Hong Kong Copyright © 1999 by John Wiley & Sons, Inc. All rights reserved. htm About Wiley InterScience | About Wiley | Privacy | Terms & Conditions Copyright © 1999-2008John Wiley & Sons, Inc.

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