Dynamics of Soliton Pulse Inside Optical Fiber

Chakresh kumar; Rahul Kumar; Deepjyoti Das

doi:doi:10.11648/j.ajop.20130102.11

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Dynamics of Soliton Pulse Inside Optical Fiber

Chakresh kumar, Rahul Kumar, Deepjyoti Das

Published in American Journal of Optics and Photonics (Volume 1, Issue 2)

Received: 13 May 2013 Accepted: 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), 2024. 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.

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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

Chakresh kumar

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

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

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

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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

Copy | Download

@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}
}

Copy | Download

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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