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Morey, Distributed fiber grating sensors, Proc. , IREE Australia, Sydney, p. 285, 1990. 29. A. D. Kersey, T. A. Berkoff, and W. W. Morey, Fiber-grating based strain sensor with phase sensitive detection, Proc. SPIE, 1777, p. 61, 1992. 30. D. A. Jackson, A. B. Lobo Ribeiro, L. Reekie, and J. L. , 18, p. 1192, 1993. 31. E. W. Saaski, J. C. Hartl, G. L. Mitchell, R. A. Wolthuis, and M. A. Afromowitz, A family of fiber optic sensor using cavity resonator microshifts, Proc. 4th Intl. Conf. Optical Fiber Sensors, Tokyo, 1986.

164, 1988. Y. F. Li and J. W. Lit, Temperature effects of a multimode biconical fiber coupler, Appl. , 25, p. 1765, 1986. Y. Murakami and S. Sudo, Coupling characteristics measurements between curved waveguides using a two core fiber coupler, Appl. , 20, p. 417, 1981. 38 Udd 17. D. A. Nolan, P. E. Blaszyk, and E. , Wiley, New York, 1991. 18. J. W. Berthold, W. L. Ghering, and D. Varshneya, Design and characterization of a high temperature, fiber optic pressure transducer, IEEE J. , LT-5, p. 1, 1987.

If a split detector is used with a photomask arranged so that the opaque and transparent line pairs on the mask in front of the split detector match the interference pattern periodicity and are 90 out of phase on the detector faces, sine and cosine outputs result. These outputs may be processed using quadrature demodulation electronics, as shown in Fig. 35. The result is a direct measure of the phase difference. Further improvements on these techniques have been made; notably the phase-generated carrier approach shown in Fig.

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