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Novel dynamics of the Fokas-Lenells model in Birefringent fibers applying different integration algorithms Cover

Novel dynamics of the Fokas-Lenells model in Birefringent fibers applying different integration algorithms

Open Access
|Jun 2024

Figures & Tables

Fig. 1

Behaviour of ψ1 for 



q=12
q = \frac{1}{2}


, r = 3, p = −1, p1 = 7, p2 = 2, λ0 = 0, λ1 = ɛ = 1: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.
Behaviour of ψ1 for q=12 q = \frac{1}{2} , r = 3, p = −1, p1 = 7, p2 = 2, λ0 = 0, λ1 = ɛ = 1: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.

Fig. 2

Plot of solution ψ5 for p = λ0 = 0, λ1 = p1 = r = q = ɛ = 1, p2 = 2: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.
Plot of solution ψ5 for p = λ0 = 0, λ1 = p1 = r = q = ɛ = 1, p2 = 2: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.

Fig. 3

Graphical representation of ψ6 for M = 0, L = N = r = p1 = ɛ = 1, p2 = k = 2: (a,b,c) cubic wave form, and (d,e,f) 2D wave pattern.
Graphical representation of ψ6 for M = 0, L = N = r = p1 = ɛ = 1, p2 = k = 2: (a,b,c) cubic wave form, and (d,e,f) 2D wave pattern.

Fig. 4

Outlook of solution ψ7 for q = B = λ = p1 = p2 = β1 = γ = ɛ = 1, r = 2: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.
Outlook of solution ψ7 for q = B = λ = p1 = p2 = β1 = γ = ɛ = 1, r = 2: (a,b,c) cubical wave pattern, and (d,e,f) planner wave pattern.
Language: English
Page range: 1 - 12
Submitted on: Sep 3, 2023
Accepted on: Dec 8, 2023
Published on: Jun 2, 2024
Published by: Harran University
In partnership with: Paradigm Publishing Services
Publication frequency: 2 issues per year

© 2024 Mst. Ishrat Jahan, Mohammad Safi Ullah, Harun-Or Roshid, Zillur Rahman, Rabeya Akter, published by Harran University
This work is licensed under the Creative Commons Attribution 4.0 License.