Download Applications of Nonlinear Fiber Optics by Govind Agrawal PDF

By Govind Agrawal

ISBN-10: 0120451441

ISBN-13: 9780120451449

Because the box grew, Agrawal determined to separate this article off from his Nonlinear Fiber Optics, that is extra occupied with the discipline's basics. This version is meant for senior undergraduates, graduate scholars, engineers and technicians within the telecommunications undefined, and scientists operating with fiber optics and optical communications. It covers the construction blocks of light-wave expertise - fiber-based gratings, couplers, and interferometers - in addition to amplifiers and lasers made utilizing rare-earth-doped fibers; pulse-compression recommendations; fiber-optic verbal exchange platforms; and soliton-based transmission schemes.

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These equations then reduce to Eqs. 20 Transmitted power as a function of input peak power for (a) δ 0 and (b) 1 5 cm 1 . Experimental data (solid circles) are compared with coupled-mode theory (open circles). Dashed lines shows the behavior expected in the absence of c 1997 IEEE) nonlinear effects. (After Ref. [135] ­ with the only difference that both z derivatives have the same sign. 2. 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.

Doubling of the arrival time for δ close to 900 m 1 shows that the pulse speed was only 50% of that expected in the absence of the grating. This result is in complete agreement with the prediction of coupledmode theory. 10 can be attributed mostly to the grating-induced GVD effects in Eq. 26). The large broadening observed near the stop-band edge is due to an increase in β g2 . Slight compression near δ 1200 m 1 is due to a small amount of SPM that chirps the pulse. Indeed, it was necessary to include the γ term in Eqs.

The large broadening observed near the stop-band edge is due to an increase in β g2 . Slight compression near δ 1200 m 1 is due to a small amount of SPM that chirps the pulse. Indeed, it was necessary to include the γ term in Eqs. 12) to fit the experimental data. The nonlinear effects became quite significant at higher power levels. We turn to this issue next. 4 CW Nonlinear Effects Wave propagation in a nonlinear, one-dimensional, periodic medium has been studied in several different contexts [67]–[87].

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