Scattering of a solitary pulse on a local defect or breather
Panayotis G. Kevrekidis, Boris A. Malomed, H. E. Nistazakis, Dimitri J. Frantzeskakis, A. Saxena, A. R. Bishop
Abstract
A model is introduced to describe guided propagation of a linear or nonlinear pulse which encounters a localized nonlinear defect, that may be either static or breather-like one (the model with the static defect applies to an optical pulse in a long fiber link with an inserted additional section of a nonlinear fiber). In the case when the host waveguide is linear, the pulse has a Gaussian shape. In that case, an immediate result of its interaction with the nonlinear defect can be found in an exact analytical form, amounting to transformation of the incoming Gaussian into an infinite array of overlapping Gaussian pulses. Further evolution of the array in the linear host medium is found numerically by means of the Fourier transform. An important ingredient of the linear medium is the third-order dispersion, that eventually splits the array into individual pulses. If the host medium is nonlinear, the input pulse is taken as a fundamental soliton. The soliton is found to be much more resistant to the action of the nonlinear defect than the Gaussian pulse in the linear host medium. In this case, the third-order-dispersion splits the soliton proper and wavepackets generated by the action of the defect.
Create a lesson
Related papers
Aberration stabilized light bullets in normal dispersion injected Kerr resonators
Yannick Fleck, Thomas G. Seidel, Jesús Yelo-Sarrión et al.
Rate-selective synchronization in switching networks: when timing meets structure
Russell Jeter, Angelo Boateng, Maurizio Porfiri et al.
On the Time-Domain Waveforms Leading to Frequency Comb Spectra
Madhurendra Mishra, Adarsh Ganesan
Oscillatory instability of subcritical stationary solutions in the parametrically driven, damped nonlinear Dirac equation
Fernando Carreño-Navas
Curvature and confinement: robustness of dryland vegetation patterns on sloped, undulating terrain
Timothy V Roberts, Punit Gandhi, Mary Silber
Dirac Equations With All Possible Combinations of Scalar-Scalar, Vector-Vector and Pseudoscalar-Pseudoscalar Interactions
Avinash Khare, Fred Cooper, John F. Dawson et al.