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Propagation caracteristics of chirped Vector Soliton in birefringent optical fibers with variable coefficients in the presence of third order dispersion Siham AZIEZ

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Numéro 26

Propagation caracteristics of chirped Vector Soliton in birefringent optical fibers with variable coefficients in the presence of third order dispersion

Siham AZIEZ1and Derradji BAHLOUL2

1Research Center in Industrial Technologies CRTI, P. O. Box 64, Cheraga 16014, Algiers/ Thin Films and Applications Unit - (UDCMA) -Setif- Algeria

2 Département de physique, Faculté des Sciences,Université Hadj-Lakhdar de Batna, 1 Avenue Boukhlouf Mohamed El Hadi, Batna 05000, Algeria

[email protected] POSTER- AZIEZ Siham

Abstract

WE study in this work, the propagation characteristics of chirped vector solitons in optical fiber systems using the compact split step Padé scheme (CSSPS). This study is done in the case of variable coefficients and the presence of third order dispersion. A negative chirp makes the soliton broadening, while; a positive chirp leads to a soliton compression. The effect of chirp on the soliton temporal width of an amplification system (σ>0) is greaterthan that in a loss system (σ<0). In the presence of third order dispersion, we note an increase of the pulse width with an asymmetric oscillation on the trailing edge. In the same time, we note a shift of the center of the two components of the one managed chirped vector soliton along the propagation distance.

Keywords: Vector soliton, Chirped soliton, Optical fibers, compact split step Padé scheme, Coupled higher-order nonlinear Schrodinger equations, Dispersion management, nonlinearity management, temporal waveform.

References:

[1] -GovindAgrawal, ’Nonlinear Fiber Optics’, Academic Press, 2007.

[2] A. Hasegawa, Y. Kodama, “Solitons in Optical Communications”, Clarendon Press,Oxford, 1995.

[3] A. Hasegawa, “Theory of information transfer in optical fibers: a tutorial review”,Optical Fiber Technology 10 (2004) 50–170

[4] - MoussaSmadi, Derradji Bahloul “A compact split step Padé scheme for higher- order nonlinear Schrödinger equation (HNLS) with power law nonlinearity and fourth order dispersion.”,Comput. Phys. Commun. 182 (2011) 366–371

[5] SihamAziez, MoussaSmadi, Derradji Bahloul“Semi-Implicit Operator Splitting Padé Method For Vector HNLS Solitons.”,AIP Conference Proceedings 09/2008;

1047(1). DOI:10.1063/1.2999940

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Numéro 26

[6]HongjunZheng, Chongqing Wu,Zhi Wang, Huishan Yu, Shanliang Liu, Xin Li,

‘Propagation characteristics of chirped soliton in periodic distributed amplification systems with variable coefficients’, optik (2012),123, pp. 818-822.

[7] Zhenli. Xu, Jingson He and Houde Han, ‘Semi-implicit operator splitting Padé method for higher-order nonlinear Schrodinger equations’, Applied Mathematics and computation , 2006, Vol 179, Issue 2, pp. 596-605.

[8] Darren Rand, Ivan Glesk, Camille-Sophie Brès, Daniel A. Nolan, Xin Chen, Joohyun Koh, Jason W. Fleischer, Ken Steiglitz, and Paul R. Prucnal, ”Observation of Temporal Vector Soliton Propagation and Collision in Birefringent Fiber”, DOI:

10.1103/PhysRevLett.98.053902.

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