By Anjan Biswas, Swapan Konar

Regardless of awesome advancements within the box, a close therapy of non-Kerr legislation media has no longer been released. creation to non-Kerr legislations Optical Solitons is the 1st e-book dedicated solely to optical soliton propagation in media that possesses non-Kerr legislations nonlinearities.After an creation to the fundamental good points of fiber-optic communications, the booklet outlines the nonlinear Schr?dinger equation (NLSE), conserved amounts, and adiabatic dynamics of soliton parameters. It then derives the NLSE for Kerr legislations nonlinearity from simple ideas, the inverse scattering remodel, and the 1-soliton resolution. The e-book additionally explains the variational precept and Lie rework. In every one case of non-Kerr legislations solitons, the authors boost soliton dynamics, evaluated integrals of movement, and adiabatic dynamics of soliton parameters in keeping with multiple-scale perturbation idea. The booklet explores intra-channel collision of optical solitons in either Hamiltonian and non-Hamiltonian style perturbations. moreover, it examines the stochastic perturbation of optical solitons, the corresponding Langevin equations, and optical couplers, via an advent to optical bullets.Establishing a foundation in an incredible but insufficiently documented topic, advent to non-Kerr legislation Optical Solitons can assist gasoline advances in optical conversation structures.

**Read or Download Introduction to non-Kerr Law Optical Solitons (Chapman & Hall CRC Applied Mathematics & Nonlinear Science) PDF**

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**Additional info for Introduction to non-Kerr Law Optical Solitons (Chapman & Hall CRC Applied Mathematics & Nonlinear Science)**

**Sample text**

69) 1. 70) has a solution q (0) that is taken as a solitary wave or a soliton solution. 71) where, θi for 1 ≤ i ≤ m are the so-called fast variables while T = t and X = x are the slow variables, and Pl for 1 ≤ l ≤ N is the parameter that depends on the slow variables. In many problems, only one fast variable, namely θ = x− P1 t in the unperturbed problem, is needed. One can generalize θ to satisfy ∂θ/∂x = 1 and ∂θ/∂t = −P1 and can use P1 = P1 ( X, T) to remove the secular terms. 71), is a quasi-stationary solution and one can write q = qˆ (θ, X, T, ).

This method has several advantages for studying solitons in the nonlinear optics community. Some of these advantages are [38] 1. This method is applicable to a perturbation problem for which the unperturbed system may not be integrable. Also, this method only requires that the unperturbed system admits a well-defined solution, such as a soliton, although this method has limitations. 2. It is a universal method that is suitable for equations in any dimensions with external forces and potentials.

166) where q nx = ∂n q /∂x n . 167) P1: Binaya Dash October 5, 2006 12:36 C6382 C6382˙Book Kerr Law Nonlinearity 51 where ψnx = ∂n ψ/∂x n . Note that d/d x = q x . 169) for example, X[q , q ∗ ] = (i/2)q xx + i|q |2 q . 170). Also, define the space χ (0) [[q , q ∗ ]] as the set of polynomials that satisfy the relation X[e iθ q , e −iθ q ∗ ] = e iθ X[q , q ∗ ]. 94) belong to χ (0) [[q , q ∗ ]]. 171) n=0 where Xn is a homogenous polynomial of (q , q ∗ , q x , q x∗ . ) and Deg(Xn+1 ) = Deg( Xn ) + 1.