By Robert Boyd (Auth.)
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Extra resources for Contemporary Nonlinear Optics
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For T E waves (^-polarized) and the yth medium this reduces to solving the equation . 2 3 ^ £ y ( x ) - q k%(x) + k\E y(x) = 0. (15) N o t e the change in notation adopted here to reduce the complexity of the suband superscripts: Ey and ocy denote the y-polarized field (Ey) and nonlinearity ((Xyy) in the yth medium. The simplest case occurs for one or two nonlinear bounding media, and a film whose refractive index is independent of intensity. ) For a nonlinear cladding (χ < 0, γ = c), the transverse field distributions are given by [94,95] E ^ = K a ^ r a ^2c( c)>0, u (16a) V c cosh[^ c /c(x c - x)] EG(x)= /Λ · ur li a (16b) V | a c | sinh[(?
C. Walker, C. N . Ironside, and T. J. Cullen, Optics Commun. 61,277(1987). Κ. Κ. Anderson, P h . D . Thesis, M. I. T. (1989); M. J. Lagasse, Κ. K. Anderson, C. A. W a n g , H. A. H a u s , and J. G. Fujimoto, Appl. Phys. Lett. 56, 417 (1990). K. D e L o n g and G. I. Stegeman, "Dispersion of the two p h o t o n absorption p a r a m e t e r for all-optical switching," Appl. Phys. Lett. 57, 2062 (1990). R. Hoffe and J. Chrostowski, Opt. Commun. 57, 34 (1986). S. Trillo, S. Wabnitz, R. H. Stolen, G.
Contemporary Nonlinear Optics by Robert Boyd (Auth.)