Applied optics and optical engineering. Vol. I: Light. Its by R. Kingslake

By R. Kingslake

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W. Morey, and J. P. Waters, Electron. Lett. 26, 1829 (1990). [26] V. Mizrahi, S. La Rochelle, and G. I. Stegeman, Phys. Rev. A 43, 433 (1991). [27] S. E. Kanellopoulos, V. A. Handerek, H. Jamshidi, and A. J. Rogers, IEEE Photon. Technol. Lett. 3, 244 (1991). [28] S. Legoubin, E. Fertein, M. Douay, P. Bernage, P. Nidy, F. Bayon, and T. Georges, Electron. Lett. 27, 1945 (1991). [29] P. St. J. Russell, L. J. Poyntz-Wright, and D. P. Hand, Proc. SPIE 1373, 126 (1991). [30] G. Meltz and W. W. Morey, Proc.

10) Using Eq. 8), the GVD parameter β2g can be shown to be the same as in Eq. 26). Several features of Eq. 9) are noteworthy when this equation is compared with the standard NLS equation. First, the variable U represents the amplitude of the envelope associated with the Bloch wave formed by a superposition of A f and Ab . Second, the parameters β2g and γg are not constants but depend on the speed-reduction factor v. Both increase as v decreases and become infinite at the edges of the stop band where v = 0.

A. M. Streltsov and N. F. Borrelli, J. Opt. Soc. Am. B 19, 2496 (2002). A. Saliminia, N. T. Nguyen, M. C. Nadeau, S. Petit, S. L. Chin, and R. Vall´ee, J. Appl. Phys. 93, 3724 (2003). H. Zhang, S. M. Eaton, and P. R. Herman, Opt. Express 14, 4826 (2006). Y. Kondo, K. Nouchi, T. Mitsuyy, M. Watanabe, P. G. Kanansky, and K. Hirao, Opt. Lett. 24, 646 (1999). S. J. Mihailov, C. W. Smelser, D. Grobnic, R. B. Walker, P. Lu, H. Ding, and J. Unruh, J. Lightwave Technol. 22, 94-100 (2004). C. W. Smelser, S.

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