A partial coupling power of single mode fiber fusion

Coupled fibers are successfully fabricated by injecting hydrogen flow at 1 bar and fused slightly by unstable torch flame in the range of 800-1350C. Optical parameters may vary significantly over wide range physical properties. Coupling coefficient and refractive index are estimated from the experim...

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Main Authors: Toto, Saktioto, Ali, Jalil, Abd Rahman, Rosly, Fadhali, Mohammed, Zainal, Jasman
Format: Article
Language:English
Published: 2007
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Online Access:http://eprints.utm.my/id/eprint/5880/1/A_PARTIAL_COUPLING_POWER_OF_SINGLE_MODE_FIBER_FUSION.pdf
http://eprints.utm.my/id/eprint/5880/
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spelling my.utm.58802010-06-01T15:36:06Z http://eprints.utm.my/id/eprint/5880/ A partial coupling power of single mode fiber fusion Toto, Saktioto Ali, Jalil Abd Rahman, Rosly Fadhali, Mohammed Zainal, Jasman QC Physics Coupled fibers are successfully fabricated by injecting hydrogen flow at 1 bar and fused slightly by unstable torch flame in the range of 800-1350C. Optical parameters may vary significantly over wide range physical properties. Coupling coefficient and refractive index are estimated from the experimental result of the coupling ratio distribution from 1% to 75%. The change of structural and geometrical fiber affects the normalized frequency (V) even for single mode fibers. Coupling ratio as a function of coupling coefficient and separation of fiber axis changes with respect to V at coupling region. V is derived from radius, wavelength and refractive index parameters. Parametric variations are performed on the left and right hand side of the coupling region. At the center of the coupling region V is assumed constant. A partial power is modeled and derived using V, normalized lateral phase constant (ư), and normalized lateral attenuation constant, (w) through the second kind of modified Bessel function of the / order, which obeys the normal mode, LP01 and normalized propagation constant (b). Total power is maintained constant in order to comply with the energy conservation law. The power is integrated through V, ư and w over the pulling length range of 7500-9500μm for 1-D where radial and angle directions are ignored. The core radius of fiber significantly affects V and power partially at coupling region rather than wavelength and refractive index of core and cladding. This model has power phenomena in transmission and reflection for industrial application of coupled fibers. 2007-12 Article PeerReviewed application/pdf en http://eprints.utm.my/id/eprint/5880/1/A_PARTIAL_COUPLING_POWER_OF_SINGLE_MODE_FIBER_FUSION.pdf Toto, Saktioto and Ali, Jalil and Abd Rahman, Rosly and Fadhali, Mohammed and Zainal, Jasman (2007) A partial coupling power of single mode fiber fusion. International workshop and conference on photonics and nanotechnology . p. 1.
institution Universiti Teknologi Malaysia
building UTM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Teknologi Malaysia
content_source UTM Institutional Repository
url_provider http://eprints.utm.my/
language English
topic QC Physics
spellingShingle QC Physics
Toto, Saktioto
Ali, Jalil
Abd Rahman, Rosly
Fadhali, Mohammed
Zainal, Jasman
A partial coupling power of single mode fiber fusion
description Coupled fibers are successfully fabricated by injecting hydrogen flow at 1 bar and fused slightly by unstable torch flame in the range of 800-1350C. Optical parameters may vary significantly over wide range physical properties. Coupling coefficient and refractive index are estimated from the experimental result of the coupling ratio distribution from 1% to 75%. The change of structural and geometrical fiber affects the normalized frequency (V) even for single mode fibers. Coupling ratio as a function of coupling coefficient and separation of fiber axis changes with respect to V at coupling region. V is derived from radius, wavelength and refractive index parameters. Parametric variations are performed on the left and right hand side of the coupling region. At the center of the coupling region V is assumed constant. A partial power is modeled and derived using V, normalized lateral phase constant (ư), and normalized lateral attenuation constant, (w) through the second kind of modified Bessel function of the / order, which obeys the normal mode, LP01 and normalized propagation constant (b). Total power is maintained constant in order to comply with the energy conservation law. The power is integrated through V, ư and w over the pulling length range of 7500-9500μm for 1-D where radial and angle directions are ignored. The core radius of fiber significantly affects V and power partially at coupling region rather than wavelength and refractive index of core and cladding. This model has power phenomena in transmission and reflection for industrial application of coupled fibers.
format Article
author Toto, Saktioto
Ali, Jalil
Abd Rahman, Rosly
Fadhali, Mohammed
Zainal, Jasman
author_facet Toto, Saktioto
Ali, Jalil
Abd Rahman, Rosly
Fadhali, Mohammed
Zainal, Jasman
author_sort Toto, Saktioto
title A partial coupling power of single mode fiber fusion
title_short A partial coupling power of single mode fiber fusion
title_full A partial coupling power of single mode fiber fusion
title_fullStr A partial coupling power of single mode fiber fusion
title_full_unstemmed A partial coupling power of single mode fiber fusion
title_sort partial coupling power of single mode fiber fusion
publishDate 2007
url http://eprints.utm.my/id/eprint/5880/1/A_PARTIAL_COUPLING_POWER_OF_SINGLE_MODE_FIBER_FUSION.pdf
http://eprints.utm.my/id/eprint/5880/
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score 13.160551