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Optoelectronic enhancement of the Sagnac effect in a ring resonator and related effect of directional bistability
1.For a comprehensive review, see E. Post, Rev. Mod. Phys. 39, 475 (1967);
1.J. Anandan, Phys. Rev. D 24, 338 (1981).
2.F. Aronowitz, Proc. SPIE 157, 2 (1978);
2.T. A. Dorschner, H. Haus, M. Holz, I. W. Smith, and H. Statz, IEEE J. Quantum Electron. QE‐16, 1376 (1980);
2.G. A. Sanders, M. G. Prentiss, and S. Ezekiel, Opt. Lett. 6, 569 (1981).
3.Proc. Soc. Photo‐Opt. Instrum. Eng. 157 “Laser Inertial Rotation Sensors,” San Diego, CA, 1978. Fiber‐Optic Rotation Sensors and Related Technologies, edited by S. Ezekiel and H. J. Arditty (Springer, New York, 1982).
4.A. E. Kaplan and P. Meystre, Opt. Lett. 6, 590 (1981);
4.see also in Fiberoptic Rotation Sensors and Related Technologies, edited by S. Ezekiel and H. J. Arditty (Springer̀, New York, 1982), p. 375.
5.A. E. Kaplan and P. Meystre, Opt. Commun. 40, 229 (1982);
5.see also in Fiber‐Optic Rotation Sensors & Related Technologies, edited by S. Ezekiel and H. J. Arditty (Springer, New York, 1982) p. 375.
6.The use of Faraday rotators of various kinds in application to bias in laser gyro was discussed by I. W. Smith and T. A. Dorschner, Proc. SPIE 157, 21 (1978).
7.A. E. Kaplan (unpublished).
8.L. A. Hackel, R. P. Hackel, and S. Ezekiel, Metrologia 13, 141 (1977).
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