Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion

Graphene is at the center of a significant research effort for ultrafast photonics due to its unique optical properties. Here, we demonstrated the generation of stretched and soliton femtosecond mode-locking pulses in an erbium doped fiber laser (EDFLs) by using graphene saturable absorber and manag...

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Main Authors: Ahmed, Mahmoud Hazzaa M., Al-Masoodi, Ahmed Hasan Hamood, Yasin, Moh, Arof, Hamzah, Harun, Sulaiman Wadi
Format: Article
Published: Elsevier 2017
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Online Access:http://eprints.um.edu.my/19729/
https://doi.org/10.1016/j.ijleo.2017.03.011
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Institution: Universiti Malaya
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spelling my.um.eprints.197292019-08-27T06:44:13Z http://eprints.um.edu.my/19729/ Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion Ahmed, Mahmoud Hazzaa M. Al-Masoodi, Ahmed Hasan Hamood Yasin, Moh Arof, Hamzah Harun, Sulaiman Wadi QC Physics TK Electrical engineering. Electronics Nuclear engineering Graphene is at the center of a significant research effort for ultrafast photonics due to its unique optical properties. Here, we demonstrated the generation of stretched and soliton femtosecond mode-locking pulses in an erbium doped fiber laser (EDFLs) by using graphene saturable absorber and managing the net cavity dispersion. The novelty of this work arises due to the simple fabrication of the graphene SA and the realization of two types of mode-locking pulse by manipulating the cavity dispersion. At total cavity dispersion of −0.028 ps2, stretched pulses train was successfully obtained. The laser has a pulse width of 750 fs at repetition rate of 35.1 MHz and pulse energy of 0.054 nJ at maximum output power of 1.9 mW. By varying the net cavity dispersion so that the anomalous dispersion has been achieved with total dispersion of −0.3 ps2, soliton mode locked pulse train was successfully obtained. The laser has a pulse width of 820 fs at repetition rate of 11.5 MHz and pulse energy of 0.42 nJ at output power of 4.85 mW. These results make the proposed EDFLs suitable for applications in optical communications, metrology, environmental sensing, and biomedical diagnostics. Elsevier 2017 Article PeerReviewed Ahmed, Mahmoud Hazzaa M. and Al-Masoodi, Ahmed Hasan Hamood and Yasin, Moh and Arof, Hamzah and Harun, Sulaiman Wadi (2017) Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion. Optik, 138. pp. 250-255. ISSN 0030-4026 https://doi.org/10.1016/j.ijleo.2017.03.011 doi:10.1016/j.ijleo.2017.03.011
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 QC Physics
TK Electrical engineering. Electronics Nuclear engineering
spellingShingle QC Physics
TK Electrical engineering. Electronics Nuclear engineering
Ahmed, Mahmoud Hazzaa M.
Al-Masoodi, Ahmed Hasan Hamood
Yasin, Moh
Arof, Hamzah
Harun, Sulaiman Wadi
Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
description Graphene is at the center of a significant research effort for ultrafast photonics due to its unique optical properties. Here, we demonstrated the generation of stretched and soliton femtosecond mode-locking pulses in an erbium doped fiber laser (EDFLs) by using graphene saturable absorber and managing the net cavity dispersion. The novelty of this work arises due to the simple fabrication of the graphene SA and the realization of two types of mode-locking pulse by manipulating the cavity dispersion. At total cavity dispersion of −0.028 ps2, stretched pulses train was successfully obtained. The laser has a pulse width of 750 fs at repetition rate of 35.1 MHz and pulse energy of 0.054 nJ at maximum output power of 1.9 mW. By varying the net cavity dispersion so that the anomalous dispersion has been achieved with total dispersion of −0.3 ps2, soliton mode locked pulse train was successfully obtained. The laser has a pulse width of 820 fs at repetition rate of 11.5 MHz and pulse energy of 0.42 nJ at output power of 4.85 mW. These results make the proposed EDFLs suitable for applications in optical communications, metrology, environmental sensing, and biomedical diagnostics.
format Article
author Ahmed, Mahmoud Hazzaa M.
Al-Masoodi, Ahmed Hasan Hamood
Yasin, Moh
Arof, Hamzah
Harun, Sulaiman Wadi
author_facet Ahmed, Mahmoud Hazzaa M.
Al-Masoodi, Ahmed Hasan Hamood
Yasin, Moh
Arof, Hamzah
Harun, Sulaiman Wadi
author_sort Ahmed, Mahmoud Hazzaa M.
title Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
title_short Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
title_full Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
title_fullStr Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
title_full_unstemmed Stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
title_sort stretched and soliton femtosecond pulse generation with graphene saturable absorber by manipulating cavity dispersion
publisher Elsevier
publishDate 2017
url http://eprints.um.edu.my/19729/
https://doi.org/10.1016/j.ijleo.2017.03.011
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