Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations
In this article, the collective variable method to study two types of the Chen–Lee–Liu (CLL) equations, is employed. The CLL equation, which is also the second member of the derivative nonlinear Schrödinger equations, is known to have vast applications in optical fibers, in particular. More specific...
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De Gruyter
2021
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oai:doaj.org-article:fa7c6c7090374b69b13341072adb6f4b2021-12-05T14:11:02ZOptical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations2391-547110.1515/phys-2021-0065https://doaj.org/article/fa7c6c7090374b69b13341072adb6f4b2021-10-01T00:00:00Zhttps://doi.org/10.1515/phys-2021-0065https://doaj.org/toc/2391-5471In this article, the collective variable method to study two types of the Chen–Lee–Liu (CLL) equations, is employed. The CLL equation, which is also the second member of the derivative nonlinear Schrödinger equations, is known to have vast applications in optical fibers, in particular. More specifically, a consideration to the classical Chen–Lee–Liu (CCLL) and the perturbed Chen–Lee–Liu (PCLL) equations, is made. Certain graphical illustrations of the simulated numerical results that depict the pulse interactions in terms of the soliton parameters are provided. Also, the influential parameters in each model that characterize the evolution of pulse propagation in the media, are identified.Alrashed ReyoufAlshaery Aisha AbduAlkhateeb SadahDe Gruyterarticlecll equationsperturbation termcollective variables methodsolitonsPhysicsQC1-999ENOpen Physics, Vol 19, Iss 1, Pp 559-567 (2021) |
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cll equations perturbation term collective variables method solitons Physics QC1-999 |
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cll equations perturbation term collective variables method solitons Physics QC1-999 Alrashed Reyouf Alshaery Aisha Abdu Alkhateeb Sadah Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
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In this article, the collective variable method to study two types of the Chen–Lee–Liu (CLL) equations, is employed. The CLL equation, which is also the second member of the derivative nonlinear Schrödinger equations, is known to have vast applications in optical fibers, in particular. More specifically, a consideration to the classical Chen–Lee–Liu (CCLL) and the perturbed Chen–Lee–Liu (PCLL) equations, is made. Certain graphical illustrations of the simulated numerical results that depict the pulse interactions in terms of the soliton parameters are provided. Also, the influential parameters in each model that characterize the evolution of pulse propagation in the media, are identified. |
format |
article |
author |
Alrashed Reyouf Alshaery Aisha Abdu Alkhateeb Sadah |
author_facet |
Alrashed Reyouf Alshaery Aisha Abdu Alkhateeb Sadah |
author_sort |
Alrashed Reyouf |
title |
Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
title_short |
Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
title_full |
Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
title_fullStr |
Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
title_full_unstemmed |
Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations |
title_sort |
optical solitons via the collective variable method for the classical and perturbed chen–lee–liu equations |
publisher |
De Gruyter |
publishDate |
2021 |
url |
https://doaj.org/article/fa7c6c7090374b69b13341072adb6f4b |
work_keys_str_mv |
AT alrashedreyouf opticalsolitonsviathecollectivevariablemethodfortheclassicalandperturbedchenleeliuequations AT alshaeryaishaabdu opticalsolitonsviathecollectivevariablemethodfortheclassicalandperturbedchenleeliuequations AT alkhateebsadah opticalsolitonsviathecollectivevariablemethodfortheclassicalandperturbedchenleeliuequations |
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1718371455257804800 |