Applications of Nonlinear Fiber Optics, Second Edition by Govind Agrawal

By Govind Agrawal

* the one publication describing functions of nonlinear fiber optics * new chapters at the most modern advancements: hugely nonlinear fibers and quantum purposes * insurance of biomedical functions * difficulties supplied on the finish of every bankruptcy the advance of latest hugely nonlinear fibers - often called microstructured fibers, holey fibers and photonic crystal fibers - is the subsequent new release expertise for all-optical sign processing and biomedical purposes. This new version has been completely up to date to include those key know-how advancements. The booklet offers sound assurance of the basics of lightwave expertise, besides fabric on pulse compression options and rare-earth-doped fiber amplifiers and lasers. The broadly revised chapters comprise details on fiber-optic communique platforms and the ultrafast sign processing innovations that utilize nonlinear phenomena in optical fibers. New fabric specializes in the purposes of hugely nonlinear fibers in components starting from wavelength laser tuning and nonlinear spectroscopy to biomedical imaging and frequency metrology. applied sciences resembling quantum cryptography, quantum computing, and quantum communications also are coated in a brand new bankruptcy. This ebook may be an awesome reference for: R&D engineers engaged on constructing subsequent new release optical parts; scientists concerned with examine on fiber amplifiers and lasers; graduate scholars and researchers operating within the fields of optical communications and quantum details. * the single booklet on tips on how to increase nonlinear fiber optic purposes * new chapters at the most modern advancements; hugely Nonlinear Fibers and Quantum purposes * assurance of biomedical functions

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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.

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