Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber

A Q-switched distributed Bragg reflector fiber laser using a graphene passive saturable absorber is proposed in a cavity consisting of a fiber Bragg grating and Faraday rotator mirror as end mirrors, together with a highly doped erbium-doped fiber as a gain source. The laser has a Q-switched thresho...

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Main Authors: Ahmad, Harith, Muhammad, F.D., Zulkifli, M.Z., Harun, Sulaiman Wadi
Format: Article
Published: Optical Society of America 2013
Subjects:
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author Ahmad, Harith
Muhammad, F.D.
Zulkifli, M.Z.
Harun, Sulaiman Wadi
author_facet Ahmad, Harith
Muhammad, F.D.
Zulkifli, M.Z.
Harun, Sulaiman Wadi
author_sort Ahmad, Harith
collection UM
description A Q-switched distributed Bragg reflector fiber laser using a graphene passive saturable absorber is proposed in a cavity consisting of a fiber Bragg grating and Faraday rotator mirror as end mirrors, together with a highly doped erbium-doped fiber as a gain source. The laser has a Q-switched threshold of about 28 mW and a tunable repetition rate of 10.4-18.0 kHz with varying pump power. The shortest pulse width obtained from the system is 3.7 <i>μ</i>s, with a maximum pulse energy and peak power of 22.2 nJ and 3.4 mW, respectively.
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spelling um.eprints-143912018-10-09T06:01:02Z http://eprints.um.edu.my/14391/ Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber Ahmad, Harith Muhammad, F.D. Zulkifli, M.Z. Harun, Sulaiman Wadi QC Physics TK Electrical engineering. Electronics Nuclear engineering A Q-switched distributed Bragg reflector fiber laser using a graphene passive saturable absorber is proposed in a cavity consisting of a fiber Bragg grating and Faraday rotator mirror as end mirrors, together with a highly doped erbium-doped fiber as a gain source. The laser has a Q-switched threshold of about 28 mW and a tunable repetition rate of 10.4-18.0 kHz with varying pump power. The shortest pulse width obtained from the system is 3.7 <i>μ</i>s, with a maximum pulse energy and peak power of 22.2 nJ and 3.4 mW, respectively. Optical Society of America 2013 Article PeerReviewed Ahmad, Harith and Muhammad, F.D. and Zulkifli, M.Z. and Harun, Sulaiman Wadi (2013) Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber. Chinese Optics Letters, 11 (7). 071401. ISSN 1671-7694, https://www.osapublishing.org/col/abstract.cfm?uri=col-11-7-071401
spellingShingle QC Physics
TK Electrical engineering. Electronics Nuclear engineering
Ahmad, Harith
Muhammad, F.D.
Zulkifli, M.Z.
Harun, Sulaiman Wadi
Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title_full Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title_fullStr Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title_full_unstemmed Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title_short Q-switched pulse generation from an all-fiber distributed Bragg reflector laser using graphene as saturable absorber
title_sort q switched pulse generation from an all fiber distributed bragg reflector laser using graphene as saturable absorber
topic QC Physics
TK Electrical engineering. Electronics Nuclear engineering
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