4.7 Article

On the quintic time-dependent coefficient derivative nonlinear Schrodinger equation in hydrodynamics or fiber optics

期刊

NONLINEAR DYNAMICS
卷 96, 期 1, 页码 229-241

出版社

SPRINGER
DOI: 10.1007/s11071-019-04786-0

关键词

Quintic time-dependent coefficient derivative nonlinear Schrodinger equation; Equivalent form; Painleve analysis; Bilinear forms; N-soliton solutions; Breathers

资金

  1. National Natural Science Foundation of China [11772017]
  2. Fundamental Research Funds for the Central Universities [50100002016105010]

向作者/读者索取更多资源

Under investigation in this paper is a quintic time-dependent coefficient derivative nonlinear Schrodinger equation for certain hydrodynamic wave packets or a medium with the negative refractive index. A gauge transformation is found to obtain the equivalent form of the equation. With respect to the wave envelope for the free water surface displacement or envelope of the electric field, Painleve integrable condition, different from that in the existing literature, is derived, with which the bilinear forms and N-soliton solutions are constructed. Asymptotic analysis illustrates that the interactions between the bright and bound solitons as well as between the bright solitons and Kuznetsov-Ma breathers are elastic with certain conditions, while some other interactions are inelastic under other conditions. Propagation paths and velocities for the solitons are both affected by the dispersion coefficient function when the relations among the coefficients are linear, or affected by the dispersion coefficient, self-steepening coefficient and cubic nonlinearity functions when the relations among the coefficients are nonlinear. Under different conditions, bell-shaped solitons can evolve into the bound solitons or Kuznetsov-Ma breathers, respectively. Interactions between the bright and parabolic (or hyperbolic) solitons are related to the dispersion coefficient, self-steepening coefficient and cubic nonlinearity functions. Compression effect on the propagation paths of the solitons, caused by the dispersion coefficient, is observed.

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