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Dynamics of Soliton Pulse Inside Optical Fiber

Received: 13 May 2013     Published: 30 May 2013
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Abstract

The main aim of this paper is to implement the combine effect of linearity and nonlinearity in optical fiber that generate a stable, undistorted pulse called “soliton”. Analysis of first, second and third order soliton pulse propagation are done by modifying the nonlinear Schrodinger equation (NLSE).Further we have found that power requirement for transmitting fundamental order soliton, second order and third order are 83.3mW, 333.3mW and 750mW respectively. In which power of 83.3mW is appropriate for soliton pulse to maintain least loss during the propagation in optical fiber.

Published in American Journal of Optics and Photonics (Volume 1, Issue 2)
DOI 10.11648/j.ajop.20130102.11
Page(s) 6-10
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2013. Published by Science Publishing Group

Keywords

Non Linear Schrodinger Equation (NLSE), Soliton, Order of Soliton, Dispersion

References
[1] Govind p. Agrawal, "Fiber optic communication systems", Second edition., John Wiley & Sons, Inc,ISBN 0-471-21571-6, 2002.
[2] G.P Agrawal, "Nonlinear fiber optics, optics and photonics "Third edition, Academic press, ISBN-10:81-312-0119-8, 2006.
[3] Linn F Mollenauer & James P Gordon , "Solitons in optical fiber, Fundamentals and application", Academic Press,ISBN 13: 978-0-12-504190-4, 2006.
Cite This Article
  • APA Style

    Chakresh kumar, Rahul Kumar, Deepjyoti Das. (2013). Dynamics of Soliton Pulse Inside Optical Fiber. American Journal of Optics and Photonics, 1(2), 6-10. https://doi.org/10.11648/j.ajop.20130102.11

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    ACS Style

    Chakresh kumar; Rahul Kumar; Deepjyoti Das. Dynamics of Soliton Pulse Inside Optical Fiber. Am. J. Opt. Photonics 2013, 1(2), 6-10. doi: 10.11648/j.ajop.20130102.11

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    AMA Style

    Chakresh kumar, Rahul Kumar, Deepjyoti Das. Dynamics of Soliton Pulse Inside Optical Fiber. Am J Opt Photonics. 2013;1(2):6-10. doi: 10.11648/j.ajop.20130102.11

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  • @article{10.11648/j.ajop.20130102.11,
      author = {Chakresh kumar and Rahul Kumar and Deepjyoti Das},
      title = {Dynamics of Soliton Pulse Inside Optical Fiber},
      journal = {American Journal of Optics and Photonics},
      volume = {1},
      number = {2},
      pages = {6-10},
      doi = {10.11648/j.ajop.20130102.11},
      url = {https://doi.org/10.11648/j.ajop.20130102.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajop.20130102.11},
      abstract = {The main aim of this paper is to implement the combine effect of linearity and nonlinearity in optical fiber that generate a stable, undistorted pulse called “soliton”. Analysis of  first, second and third order soliton pulse propagation are done by modifying the nonlinear Schrodinger equation (NLSE).Further we have found that power requirement for transmitting fundamental order soliton, second order and third order are 83.3mW, 333.3mW and  750mW respectively. In which power of 83.3mW is appropriate for soliton pulse to maintain least loss during the propagation in optical fiber.},
     year = {2013}
    }
    

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  • TY  - JOUR
    T1  - Dynamics of Soliton Pulse Inside Optical Fiber
    AU  - Chakresh kumar
    AU  - Rahul Kumar
    AU  - Deepjyoti Das
    Y1  - 2013/05/30
    PY  - 2013
    N1  - https://doi.org/10.11648/j.ajop.20130102.11
    DO  - 10.11648/j.ajop.20130102.11
    T2  - American Journal of Optics and Photonics
    JF  - American Journal of Optics and Photonics
    JO  - American Journal of Optics and Photonics
    SP  - 6
    EP  - 10
    PB  - Science Publishing Group
    SN  - 2330-8494
    UR  - https://doi.org/10.11648/j.ajop.20130102.11
    AB  - The main aim of this paper is to implement the combine effect of linearity and nonlinearity in optical fiber that generate a stable, undistorted pulse called “soliton”. Analysis of  first, second and third order soliton pulse propagation are done by modifying the nonlinear Schrodinger equation (NLSE).Further we have found that power requirement for transmitting fundamental order soliton, second order and third order are 83.3mW, 333.3mW and  750mW respectively. In which power of 83.3mW is appropriate for soliton pulse to maintain least loss during the propagation in optical fiber.
    VL  - 1
    IS  - 2
    ER  - 

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Author Information
  • Department of Electronics and Communication Engineering, Tezpur (Central) University, India

  • Department of Electronics and Communication Engineering, Tezpur (Central) University, India

  • Department of Electronics and Communication Engineering, Tezpur (Central) University, India

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