By R. E. Slusher, B. J. Eggleton (auth.), Richard E. Slusher, Benjamin J. Eggleton (eds.)
ISBN-10: 3642078672
ISBN-13: 9783642078675
ISBN-10: 3662051443
ISBN-13: 9783662051443
Nonlinear optical reviews of periodic dielectric constructions have blossomed long ago 20 years. New fabrication concepts are generating fiber grating and multidimensional photonic crystals in fabrics the place the refractive index will be assorted via gentle pulses and beams. hole solitons which could propagate at any speed from 0 to the rate of sunshine and spatial solitons that hinder the diffractive unfold of sunshine in waveguide arrays are examples of the hot phenomena defined during this booklet. Microstructured optical fibers permit regulate of the guided mode dispersion for broadband mild new release and new soliton phenomena. Many new fabrics and buildings are being built that may effect new optical units with functions in optical communications and optical facts processing. the entire above themes are addressed intimately during this book.
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Lett. 81, 3383 (1998); R. Morandotti, U. S. S. Eisenberg, and Y. Silberberg: Phys. Rev. Lett. 83, 2726 (1999) 56. N. D. Eugenieva: Phys. Rev. Lett. 87, (2001). 57. D. K. N. Christodoulides: Optics Lett. 26, (2001) 58. B. Aceves, C. Deangelis, S. Trillo, and S. Wabnitz: Optics Lett. 19, 332 1994 Part I Nonlinear Photonic Crystal Theory 2 Theory of Nonlinear Pulse Propagation in Periodic Structures A. l. 1 Introduction We consider here the propagation of intense light in a periodic structure. The models that we discuss are one-dimensional; this means that only a single spatial direction, that in which the light propagates, is relevant, and that the refractive index only depends on this spatial coordinate.
A. E. Slusher: Opt. Comm. E. Slusher, S. J. Eggleton, S. E. Sipe: Opt. Lett. 25, 749 (2000) G. J. Eggleton and N. Litchinitser: J. Opt. Soc. Am. B 15, 715 (1997) G. J. Eggleton: J. Opt. Soc. Am. B 15, 2979 (1998) S. E. Slusher: submitted to JOSA B. G. Winful et. : Appl. Phys. Lett. G. D. Cooperman: Appl. Phys. G. 1. Stegeman: Proc. A. J. Chandonnet, J. E. R. J. J. S. Shenk, in Optical Fiber Communication Conference. Vol. S. Cross and H. Kogelnik: Opt. Lett. 1, 43 (1977) B. C. Johnson, F. Bilodeau, J.
27) where L1 = L1(Q) = Vli2 + Q2. Thus, again in agreement with Fig. 1, the magnitude of the group velocity attains its largest value at the band edges, and decreases smoothly when tuning away from them. For a fiber grating with Ii = IDcm-I, we thus find that W2 ~ 2 x 105 m 2 s- 1 . 55 pm has a dispersion of roughly W2 ~ 2 X 10- 1 m 2 S-l, six orders of magnitude smaller than the dispersion of a typical fiber grating. Similar conclusions can be drawn for higher order dispersion [15], but we do not discuss this here further.
Nonlinear Photonic Crystals by R. E. Slusher, B. J. Eggleton (auth.), Richard E. Slusher, Benjamin J. Eggleton (eds.)
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