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By Bishnu Pal (Ed)
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Tech. , Vol. 17, pp. 2056-2058. , Chiang, K. , Gambling, W. A. (2001), Gain flattening of an erbium-dped fiber amplifier using a high-birefringence loop mirror, IEEE Photon. Technol. , Vol. 13, pp. 942-944. Li, T. (1995), The impact of optical amplifiers on long-distance lightwave communications, Proc. IEEE, Vol. 81, pp. 1568-1579. Mehta, M. Tech. (Optoelectronics and Optical Communication) dissertation Studies on Microstructured Optical Fibers, IIT Delhi. , Poole, S. B. and Payne, D. N. 55 μm, Electron.
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For efficient nonlinear devices utilizing the optical Kerr effect, the nonlinearity must be high and the nonlinear absorption must be low. A figure of merit FOM = n2/(βλ) can be defined as a useful metric to determine optimum compositions, where n2 is the nonlinear index and β is the nonlinear absorption. For isotropic medium, one and two photon resonant processes dominate the third-order susceptibility. For frequencies approximately half of the material resonance, two photon processes resonantly enhance the nonlinear index n2.