Numerical solutions of Maxwell’s equations for nonlinear-optical pulse propagation

A model and numerical solutions of Maxwell’s equations describing the propagation of short, solitonlike pulses in nonlinear dispersive optical media are presented. The model includes linear dispersion expressed in the time domain, a Kerr nonlinearity, and a coordinate system moving with the group velocity of the pulse. Numerical solutions of Maxwell’s equations are presented for circularly polarized and linearly polarized electromagnetic fields. When the electromagnetic fields are assumed to be circularly polarized, numerical solutions are compared directly with solutions of the nonlinear Schrodinger (NLS) equation. These comparisons show good agreement and indicate that the NLS equation provides an excellent model for short-pulse propagation. When the electromagnetic fields are assumed to be linearly polarized, the propagation of daughter pulses, small-amplitude pulses at three times the frequency of the solitonlike pulse, are observed in the numerical solution. These daughter pulses are shown to be the direct result of third harmonics generated by the main, solitonlike, pulse.

[1]  Richard W. Ziolkowski,et al.  Full-wave vector Maxwell equation modeling of the self-focusing of ultrashort optical pulses in a nonlinear Kerr medium exhibiting a finite response time , 1993 .

[2]  Allen Taflove,et al.  Computational modeling of femtosecond optical solitons from Maxwell's equations , 1992 .

[3]  K. Kunz,et al.  Finite difference time domain recursive convolution for second order dispersive materials , 1992, IEEE Antennas and Propagation Society International Symposium 1992 Digest.

[4]  A Taflove,et al.  Direct time integration of Maxwell's equations in nonlinear dispersive media for propagation and scattering of femtosecond electromagnetic solitons. , 1992, Optics letters.

[5]  A Taflove,et al.  Direct time integration of Maxwell's equations in linear dispersive media with absorption for scattering and propagation of femtosecond electromagnetic pulses. , 1991, Optics letters.

[6]  R. B. Standler,et al.  A frequency-dependent finite-difference time-domain formulation for dispersive materials , 1990 .

[7]  Hermann A. Haus,et al.  Raman response function of silica-core fibers , 1989, Annual Meeting Optical Society of America.

[8]  H. H. Chen,et al.  Nonlinear pulse propagation in the neighborhood of the zero-dispersion wavelength of monomode optical fibers. , 1986, Optics letters.

[9]  A. Hasegawa,et al.  Signal transmission by optical solitons in monomode fiber , 1981, Proceedings of the IEEE.

[10]  J. Satsuma,et al.  B Initial Value Problems of One-Dimensional self-Modulation of Nonlinear Waves in Dispersive Media (Part V. Initial Value Problems) , 1975 .

[11]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[12]  I. Malitson Interspecimen Comparison of the Refractive Index of Fused Silica , 1965 .

[13]  C. Hile Numerical Studies of Nonlinear Optical Pulse Propagation , 1993 .