2009
DOI: 10.1016/j.chaos.2007.06.024
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Solitary wave solutions for high dispersive cubic-quintic nonlinear Schrödinger equation

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Cited by 76 publications
(26 citation statements)
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“…In the case β 3 = γ 1 = 0, a dark solitary wave solution with amplitude only depending on the time was presented (Azzouzi,2014). In contrast, when β 3 = β 4 = γ 2 = 0, various types exact solution were discovered (Azzouzi, 2009, Huiqing,2009, Wenxiu,2009, Anjan,2010.…”
Section: Introductionmentioning
confidence: 99%
“…In the case β 3 = γ 1 = 0, a dark solitary wave solution with amplitude only depending on the time was presented (Azzouzi,2014). In contrast, when β 3 = β 4 = γ 2 = 0, various types exact solution were discovered (Azzouzi, 2009, Huiqing,2009, Wenxiu,2009, Anjan,2010.…”
Section: Introductionmentioning
confidence: 99%
“…In the present paper, the dispersive cubic-quintic Schrödinger equation (DCQSE) including higher-order time derivatives is studied through the exp a -function scheme. The nonlinear governing model in its dimensionless form is presented as below [25][26][27]:…”
Section: Introductionmentioning
confidence: 99%
“…where ( , ) is the slowly varying envelope of the electric field, 2 is the parameter of the group velocity dispersion, 3 and 4 are, respectively, the third-order and fourth-order dispersions, and 1 and 2 are the nonlinearity coefficients. When the higher order terms are ignored, we obtain the NLS.…”
Section: Introductionmentioning
confidence: 99%