Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation

A stable passively Q-switched erbium-doped fibre laser (EDFL) operating at 1536.5 nm is developed, using a 1 m long erbium-doped fibre as a gain medium and a simple graphene-based saturable absorber (SA). Using mechanical exfoliation, a single layer of graphene is obtained and deposited on the end f...

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Published in:Ukrainian Journal of Physical Optics
Main Author: Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
Format: Article
Language:English
Published: Institute of Physical Optics 2014
Online Access:https://www.scopus.com/inward/record.uri?eid=2-s2.0-84898002722&doi=10.3116%2f16091833%2f15%2f1%2f24%2f2014&partnerID=40&md5=c04ead842701737f35efb394c28fc237
id 2-s2.0-84898002722
spelling 2-s2.0-84898002722
Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
2014
Ukrainian Journal of Physical Optics
15
1
10.3116/16091833/15/1/24/2014
https://www.scopus.com/inward/record.uri?eid=2-s2.0-84898002722&doi=10.3116%2f16091833%2f15%2f1%2f24%2f2014&partnerID=40&md5=c04ead842701737f35efb394c28fc237
A stable passively Q-switched erbium-doped fibre laser (EDFL) operating at 1536.5 nm is developed, using a 1 m long erbium-doped fibre as a gain medium and a simple graphene-based saturable absorber (SA). Using mechanical exfoliation, a single layer of graphene is obtained and deposited on the end facet of an optical fibre ferrule, which is then connected to another ferrule to form the SA. The SA is integrated into an EDFL cavity to achieve a stable pulse train at the threshold pump power of 42.3 mW. When the pump power increases from 42.3 to 63.5 mW, the pulse train repetition rate increases from 10.3 to 32.4 kHz, while the pulse width varies from 10.7 to 31.0 μs. The highest energy, 166.2 nJ, is achieved at the pump power of 42.3 mW.
Institute of Physical Optics
16091833
English
Article
All Open Access; Gold Open Access
author Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
spellingShingle Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
author_facet Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
author_sort Saleh Z.S.; Anyi C.L.; Rahman A.A.; Ali N.M.; Harun S.W.; Manaf M.; Arof H.
title Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
title_short Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
title_full Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
title_fullStr Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
title_full_unstemmed Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
title_sort Q-switched erbium-doped fibre laser using graphene-based saturable absorber obtained by mechanical exfoliation
publishDate 2014
container_title Ukrainian Journal of Physical Optics
container_volume 15
container_issue 1
doi_str_mv 10.3116/16091833/15/1/24/2014
url https://www.scopus.com/inward/record.uri?eid=2-s2.0-84898002722&doi=10.3116%2f16091833%2f15%2f1%2f24%2f2014&partnerID=40&md5=c04ead842701737f35efb394c28fc237
description A stable passively Q-switched erbium-doped fibre laser (EDFL) operating at 1536.5 nm is developed, using a 1 m long erbium-doped fibre as a gain medium and a simple graphene-based saturable absorber (SA). Using mechanical exfoliation, a single layer of graphene is obtained and deposited on the end facet of an optical fibre ferrule, which is then connected to another ferrule to form the SA. The SA is integrated into an EDFL cavity to achieve a stable pulse train at the threshold pump power of 42.3 mW. When the pump power increases from 42.3 to 63.5 mW, the pulse train repetition rate increases from 10.3 to 32.4 kHz, while the pulse width varies from 10.7 to 31.0 μs. The highest energy, 166.2 nJ, is achieved at the pump power of 42.3 mW.
publisher Institute of Physical Optics
issn 16091833
language English
format Article
accesstype All Open Access; Gold Open Access
record_format scopus
collection Scopus
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