Robust Split-Step Fourier Methods for Simulating the Propagation of Ultra-Short Pulses in Single- and Two-Mode Optical Communication Fibers

Extensions of the split-step Fourier method (SSFM) for Schrodinger-type pulse propagation equations for simulating femto-second pulses in single- and two-mode optical communication fibers are developed and tested for Gaussian pulses. The core idea of the proposed numerical methods is to adopt an operator splitting approach, in which the nonlinear sub-operator, consisting of Kerr nonlinearity, the self-steepening and stimulated Raman scattering terms, is reformulated using Madelung transformation into a quasilinear first-order system of signal intensity and phase. A second-order accurate upwind numerical method is derived rigorously for the resulting system in the single-mode case; a straightforward extension of this method is used to approximate the four-dimensional system resulting from the nonlinearities of the chosen two-mode model. Benchmark SSFM computations of prototypical ultra-fast communication pulses in idealized single- and two-mode fibers with homogeneous and alternating dispersion parameters and also high nonlinearity demonstrate the reliable convergence behavior and robustness of the proposed approach.

[1]  R. Glowinski,et al.  A Reliable Split-Step Fourier Method for the Propagation Equation of Ultra-Fast Pulses in Single-Mode Optical Fibers , 2013, Journal of Lightwave Technology.

[2]  B. V. Leer,et al.  Towards the Ultimate Conservative Difference Scheme , 1997 .

[3]  J. Smoller Shock Waves and Reaction-Diffusion Equations , 1983 .

[4]  W. Forysiak,et al.  Single channel 320 Gbit/s short period dispersion managed transmission over 6000 km , 2000 .

[5]  Gulcin M. Muslu,et al.  A split-step Fourier method for the complex modified Korteweg-de Vries equation☆ , 2003 .

[6]  Frank Schmidt,et al.  On the Numerical Solution of Nonlinear Schr¨ odinger Type Equations in Fiber Optics , 2002 .

[7]  K. Porsezian,et al.  Ultra-short pulse propagation in birefringent fibers—the projection operator method , 2008 .

[8]  Marek Trippenbach,et al.  Propagation Technique for Ultrashort Pulses. II: Numerical Methods to Solve the Pulse Propagation Equation , 2008 .

[9]  Keith J. Blow,et al.  Theoretical description of transient stimulated Raman scattering in optical fibers , 1989 .

[10]  A. A. Amorim,et al.  Sub-two-cycle pulses by soliton self-compression in highly nonlinear photonic crystal fibers. , 2009, Optics letters.

[11]  Randall J. LeVeque,et al.  WENOCLAW: A Higher Order Wave Propagation Method , 2008 .

[12]  J. Smoller,et al.  Shock Waves and Reaction-Diffusion Equations. , 1986 .

[13]  R. Glowinski Finite element methods for incompressible viscous flow , 2003 .

[14]  R. LeVeque Finite Volume Methods for Hyperbolic Problems: Characteristics and Riemann Problems for Linear Hyperbolic Equations , 2002 .

[15]  C. Menyuk,et al.  Optimization of the split-step Fourier method in modeling optical-fiber communications systems , 2003 .

[16]  A. Gnauck,et al.  25.6-Tb/s WDM Transmission of Polarization-Multiplexed RZ-DQPSK Signals , 2008, Journal of Lightwave Technology.

[17]  E. Madelung,et al.  Quantentheorie in hydrodynamischer Form , 1927 .

[18]  W. Hager Applied Numerical Linear Algebra , 1987 .

[19]  Zhaoming Huang,et al.  Densely dispersion-managed fiber transmission system with both decreasing average dispersion and decreasing local dispersion , 2004 .

[20]  Peter D. Lax,et al.  Gibbs Phenomena , 2006, J. Sci. Comput..

[21]  Govind P. Agrawal,et al.  Nonlinear Fiber Optics , 1989 .

[22]  Edward A. Spiegel,et al.  Fluid dynamical form of the linear and nonlinear Schrödinger equations , 1980 .

[23]  B. Malomed Pulse propagation in a nonlinear optical fiber with periodically modulated dispersion: variational approach , 1997 .

[24]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .

[25]  G. Strang On the Construction and Comparison of Difference Schemes , 1968 .