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Evolution of polarization along a single‐mode fiber
1.W. Eickhoff and O. Krumpholz, Electron. Lett. 12, 405 (1976).
2.F. P. Kapron, N. F. Borelli, and D. B. Keck, IEEE Trans. Quantum Electron. QE‐8, 222 (1972).
3.W. A. Gambling, D. N. Payne, and H. Matsumara, Topical Meeting on Optical Waveguides II, Williamsburg, Va., 1977, paper TuD5 (unpublished).
4.V. Ramaswamy, R. D. Standley, and W. G. French, Ref. 3, paper TuD4.
5.V. Vali and R. Shorthill, Appl. Opt. 15, 1099 (1976).
6.M. Born and E. Wolf, Principles of Optics (Pergamon, Oxford, 1975);
6.G. N. Ramachandran and S. Ramaseshan, in Encyclopedia of Physics, edited by S. Flügge (Springer, Berlin, 1961), Vol. 25/1.
7.R. Ulrich, Opt. Lett. (to be published).
8.We define the SOP of light in the fiber by using the average polarization of the total transverse electric field in a cross section. This E is a simple superposition of the two averaged modal fields (where denotes the modes) only if these are orthogonal (Ref. 7). The latter condition is strictly satisfied if the transverse index distribution has a plane of symmetry, e.g., in an elliptical core. The orthogonality exists in good approximation also in the limit of weakly guiding fibers of nominally round index profile, where the are nearly plane waves.
9.Landoldt‐Börnstein, Zahlenwerte u. Funktionen, edited by K. A. and A. M. Hellwege (Springer‐Verlag, Berlin, 1962), Vol. II, 8, Chap. 2835.
10.W. O. Schlosser, Bell Syst. Tech. J. 51, 487 (1972).
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