Diverse solitons wave structures for coupled NLSEs in birefringent fibers with higher nonlinearities using the modified extended mapping algorithm

The solutions of Eqs. (2)–(3) may be obtained by assuming the following wave transformation:

$$\begin{aligned} \phi (z,t) =\mathcal {P}_1(\zeta )\ e^{i \varUpsilon (z,t)}, \end{aligned}$$

(9)

$$\begin{aligned}…

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