Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers

Gain clamping is demonstrated in single-pass and double-pass long wavelength band erbium-doped fiber amplifiers (L-band EDFAs). A C/L-band wavelength division multiplexing (WDM) coupler is used in single-pass system to generate a laser at 1566 nm. The gain for the amplifier is clamped at 15.5 dB wit...

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Main Authors: Harun, Sulaiman Wadi, Ahmad, Harith
Format: Article
Published: De Gruyter Open 2004
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Online Access:http://eprints.um.edu.my/19647/
http://www.physics.sk/aps/pubs/2004/aps-2004-54-1-81.pdf
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spelling my.um.eprints.196472018-10-11T08:26:50Z http://eprints.um.edu.my/19647/ Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers Harun, Sulaiman Wadi Ahmad, Harith Q Science (General) QC Physics TK Electrical engineering. Electronics Nuclear engineering Gain clamping is demonstrated in single-pass and double-pass long wavelength band erbium-doped fiber amplifiers (L-band EDFAs). A C/L-band wavelength division multiplexing (WDM) coupler is used in single-pass system to generate a laser at 1566 nm. The gain for the amplifier is clamped at 15.5 dB with gain variation of less than 0.2 dB from input signal power of -40 to -14 dBm with almost negligible noise figure penalty. However, the flatness of gain spectrum is slightly degraded due to the un-optimisation of erbium-doped fiber (EDF) length. The advantage of this configuration is that the oscillating light does not appear at the output port of the amplifier. A highly efficient gain-clamped L-band EDFA with improved noise figure characteristic is demonstrated by simply adding a broadband conventional band fiber Bragg grating (C-band FBG) in double pass system. The combination of the FBG and optical circulator has created laser in the cavity for gain clamping. By adjusting the power combination of pumps 1 and 2, the clamped gain level can be controlled. The amplifier gain is clamped at 28.1 dB from -40 to -25 dBm with gain variation of less than 0.5 dB by setting the pumps 1 and 2 at 59.5 and 50.6 mW, respectively. The gain is also flat from 1574 nm to 1604 nm with gain variation of less than 3 dB. The corresponding noise figure varies from 5.6 to 7.6 dB, which is 0.8 to 2.6 dB reduced compared to those of unclamped amplifier. De Gruyter Open 2004 Article PeerReviewed Harun, Sulaiman Wadi and Ahmad, Harith (2004) Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers. Acta Physica Slovaca, 54 (1). pp. 81-88. ISSN 1336-040X http://www.physics.sk/aps/pubs/2004/aps-2004-54-1-81.pdf
institution Universiti Malaya
building UM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Malaya
content_source UM Research Repository
url_provider http://eprints.um.edu.my/
topic Q Science (General)
QC Physics
TK Electrical engineering. Electronics Nuclear engineering
spellingShingle Q Science (General)
QC Physics
TK Electrical engineering. Electronics Nuclear engineering
Harun, Sulaiman Wadi
Ahmad, Harith
Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
description Gain clamping is demonstrated in single-pass and double-pass long wavelength band erbium-doped fiber amplifiers (L-band EDFAs). A C/L-band wavelength division multiplexing (WDM) coupler is used in single-pass system to generate a laser at 1566 nm. The gain for the amplifier is clamped at 15.5 dB with gain variation of less than 0.2 dB from input signal power of -40 to -14 dBm with almost negligible noise figure penalty. However, the flatness of gain spectrum is slightly degraded due to the un-optimisation of erbium-doped fiber (EDF) length. The advantage of this configuration is that the oscillating light does not appear at the output port of the amplifier. A highly efficient gain-clamped L-band EDFA with improved noise figure characteristic is demonstrated by simply adding a broadband conventional band fiber Bragg grating (C-band FBG) in double pass system. The combination of the FBG and optical circulator has created laser in the cavity for gain clamping. By adjusting the power combination of pumps 1 and 2, the clamped gain level can be controlled. The amplifier gain is clamped at 28.1 dB from -40 to -25 dBm with gain variation of less than 0.5 dB by setting the pumps 1 and 2 at 59.5 and 50.6 mW, respectively. The gain is also flat from 1574 nm to 1604 nm with gain variation of less than 3 dB. The corresponding noise figure varies from 5.6 to 7.6 dB, which is 0.8 to 2.6 dB reduced compared to those of unclamped amplifier.
format Article
author Harun, Sulaiman Wadi
Ahmad, Harith
author_facet Harun, Sulaiman Wadi
Ahmad, Harith
author_sort Harun, Sulaiman Wadi
title Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
title_short Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
title_full Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
title_fullStr Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
title_full_unstemmed Gain clamping in single-pass and double-pass L-band erbium-doped fiber amplifiers
title_sort gain clamping in single-pass and double-pass l-band erbium-doped fiber amplifiers
publisher De Gruyter Open
publishDate 2004
url http://eprints.um.edu.my/19647/
http://www.physics.sk/aps/pubs/2004/aps-2004-54-1-81.pdf
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score 13.159267