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C. Alferness, S. K. Korotky, and E. A. J. Marcatili, Velocitymatching techniques for integrated-optic traveling-wave switch modulators, IEEE J. , QE-20 (3): 301–309, 1984. 29. S. , Monolithic integration of waveguide polymer electrooptic modulators on VLSI circuitry, IEEE Photon. Technol. , 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.

Kogelnik and R. V. Schmidt, Switched directional couplers with alternating ⌬ͱ, IEEE J. , QE-12 (7): 396– 401, 1976. 9. S. A. Samson, R. F. Tavlykaev, and R. V. Ramaswamy, Two-section reversed ⌬ͱ switch with uniform electrodes and domain reversal, IEEE Photon. Technol. , 9 (2): 197–199, 1997. 10. S. Thaniyavarn, Modified 1 ϫ 2 directional coupler waveguide modulator, Electron. , 22 (18): 941–942, 1986. 11. S. Thaniyavarn, A synthesized digital switch using a 1 ϫ 2 directional coupler with asymmetric ⌬ͱ phase reversal electrode, Integrated and Guided-Wave Optics’88, Santa Fe, NM, Tech.

In fact, the dispersion relation for the metal-clad waveguide is identical in form to that for the step-index slab waveguide (24); it is also given by Eqs. (5) and (6), provided that β and n3 in these equations assume complex values. An important feature of the metal-clad waveguide is that it attenuates the TM0 mode much more severely than the other modes. The attenuation constant for the TM0 mode can be larger than that for the TE0 mode by several orders of magnitude (25). This property has been explored for forming polarizers and mode filters.

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