By Govind Agrawal
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Additional info for Applications of Nonlinear Fiber Optics, Second Edition (Optics and Photonics Series)
B. J. Eggleton, C. M. de Sterke, and R. E. Slusher, J. Opt. Soc. Am. B 16, 587 (1999). References                                       51 H. G. Winful, J. H. Marburger, and E. Garmire, Appl. Phys. Lett. 35, 379 (1979). H. G. Winful and G. D. Cooperman, Appl. Phys. Lett. 40, 298 (1982). H. G. Winful, Appl. Phys. Lett. 46, 527 (1985).
When a single beam excites the A1 mode at the ﬁber input, its transmission depends on its detuning δ from the Bragg wavelength and becomes quite small within the stop band centered at δ = 0. The reason is easily understood by noting that the grating transfers power to the A2 mode as light propagates inside the grating. The nonlinear effects such as SPM and XPM can affect the amount of power transferred by changing the refractive index and shifting the Bragg wavelength toward Chapter 1. 5 cm−1 .
When a dynamic grating is present, the two pulses form a gap soliton that is trapped by the grating and appears stationary in the frame of the input pulse. 018 m−1 , while keeping all other parameters the same. A similar effect was predicted as early as 1989, and the resulting solitary waves were called resonance solitons . 5 of Ref.  in the context of vector solitons forming in a birefringent ﬁber. 1 Derive Eq. 1) from the phase-matching condition in Eq. 2). 2 Use Eq. 55 μm. 45. 3 Describe the mechanism through which absorption of ultraviolet light produces changes in the refractive index of silica ﬁbers.