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Tunable multiple soliton generation in Kerr media

机译:Kerr介质中可调谐的多个孤子生成

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Optical solitons are self-confined robust beams existing in various kind of nonlinear media; their studies are of fundamental as well as technological relevance. The generation of multiple solitons has been studied using modulational instability [1], or from shock waves emerging from either bright or dark input beams propagating in dispersive media [2–5]. We propose a novel route for the generation of multiple solitons using a broad beam launched into a nonlinear medium with a modified distribution of the linear refractive index, i.e. a defect. When the size of the input beam is large compared with the defect width, defect induced modulation in the phase of the beam will result in the formation of multiple fringes. These fringes can evolve into multiple interacting solitons depending on beam excitation level. The number of fringes can be controlled by the height of the defect (i.e. index jump) as well as the ratio between the widths of the beam and of the defect. We solve the one-dimensional normalized Nonlinear Schrödinger Equation of the form equation for an input beam u(X,Z = 0) = Nu0sech(uoX), where Veff (X,Z) = − [nL2(X,Z) + 2n0nL(X,Z)], nL(X,Z) is the linear index profile, k0 = 2π/λ is the vacuum wavenumber (λ is the vacuum wavelength), p = k02wp2/2, wp is the width of the defect, equation is the normalized field, N is an integer, A is the electric field amplitude, n2 is the Kerr coefficient and n0 is the linear refractive index for the carrier; we also define the normalized coordinates Z = z/Ld (Ld = k0wp2n0) and X = x/wp
机译:光学孤子是存在于各种非线性介质中的自约束鲁棒光束。他们的研究具有基础性和技术性。已使用调制不稳定性[1]或来自在分散介质中传播的明亮或黑暗输入光束产生的冲击波研究了多孤子的产生[2-5]。我们提出了一种使用宽光束产生多重孤子的新颖方法,该光束发射到具有线性折射率即缺陷的修正分布的非线性介质中。当输入光束的大小与缺陷宽度相比较大时,缺陷在光束相位中引起的调制将导致形成多个条纹。根据光束激发水平,这些条纹可以演变成多个相互作用的孤子。条纹的数量可以通过缺陷的高度(即,折射率跳跃)以及束的宽度与缺陷的宽度之间的比率来控制。我们针对输入光束u(X,Z = 0)= Nu 0 sech(u o X)求解形式方程的一维归一化非线性Schrödinger方程,其中V eff (X,Z)= − [n L 2 (X,Z)+ 2n 0 n L (X,Z)],n L (X,Z)是线性折射率分布,k 0 =2π/λ是真空波数(λ是真空波长),p = k 0 2 w p 2 / 2, w p 是缺陷的宽度,等式是归一化场,N是整数,A是电场幅度,n 2 是克尔系数,n < inf> 0 是载体的线性折射率;我们还定义了归一化坐标Z = z / L d (L d = k 0 w p 2 n 0 )和X = x / w p

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