Spectral broadening in tight confinement geometry of a random fiber laser

We present a random Raman fiber laser pumped by a continuous-wave 1480nm source where neither a visible saturable absorber nor a fiber Bragg grating were incorporated. The backward pumping feedback loop allows a single direction of 1584nm wave propagation under tighter confinement of a dispersion co...

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Main Authors: Sarmani, Abdul Rahman, Al-Alimi, Abdulmoghni Ali Wazae, Yusoff, N. Mohd, Mahdi, Mohd Adzir
Format: Article
Language:English
Published: Elsevier BV 2022
Online Access:http://psasir.upm.edu.my/id/eprint/108727/1/Spectral%20broadening%20in%20tight%20confinement%20geometry%20of%20a%20random%20fiber%20laser.pdf
http://psasir.upm.edu.my/id/eprint/108727/
https://papers.ssrn.com/sol3/papers.cfm?abstract_id=4184332
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spelling my.upm.eprints.1087272024-10-11T08:32:13Z http://psasir.upm.edu.my/id/eprint/108727/ Spectral broadening in tight confinement geometry of a random fiber laser Sarmani, Abdul Rahman Al-Alimi, Abdulmoghni Ali Wazae Yusoff, N. Mohd Mahdi, Mohd Adzir We present a random Raman fiber laser pumped by a continuous-wave 1480nm source where neither a visible saturable absorber nor a fiber Bragg grating were incorporated. The backward pumping feedback loop allows a single direction of 1584nm wave propagation under tighter confinement of a dispersion compensating fiber (DCF). This geometry that implies a stronger Kerr-lensing effect supports two types of nonlinear broadening that were achieved in the stable output power generation. The first that agrees well to wave kinetics theory favors 1.76 to 3.53nm spectral progress. Against this flow, another type of wider broadening begun at 4.88nm before reducing gradually to 4.05nm with the increase in pump power. The former corresponds to a maximum of 6.3 times broadening ratio with respect to the pump linewidth. To date, this is the best achievement in the world at just below 1.7 W pump power level especially without utilizing pump-pulse synchronization or any external mode-locking modulations. In contrast without the tighter confinement geometry, the initiation of 4.25nm bandwidth was realized in the unstable power zone. These ascertain the double roles of dispersion compensating fiber as a stabilizing factor as well as for dispersion management. Elsevier BV 2022 Article PeerReviewed text en http://psasir.upm.edu.my/id/eprint/108727/1/Spectral%20broadening%20in%20tight%20confinement%20geometry%20of%20a%20random%20fiber%20laser.pdf Sarmani, Abdul Rahman and Al-Alimi, Abdulmoghni Ali Wazae and Yusoff, N. Mohd and Mahdi, Mohd Adzir (2022) Spectral broadening in tight confinement geometry of a random fiber laser. Optical and Quantum Electronics, 55 (8). pp. 1-15. ISSN 0306-8919; ESSN: 1572-817X https://papers.ssrn.com/sol3/papers.cfm?abstract_id=4184332 10.2139/ssrn.4184332
institution Universiti Putra Malaysia
building UPM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Putra Malaysia
content_source UPM Institutional Repository
url_provider http://psasir.upm.edu.my/
language English
description We present a random Raman fiber laser pumped by a continuous-wave 1480nm source where neither a visible saturable absorber nor a fiber Bragg grating were incorporated. The backward pumping feedback loop allows a single direction of 1584nm wave propagation under tighter confinement of a dispersion compensating fiber (DCF). This geometry that implies a stronger Kerr-lensing effect supports two types of nonlinear broadening that were achieved in the stable output power generation. The first that agrees well to wave kinetics theory favors 1.76 to 3.53nm spectral progress. Against this flow, another type of wider broadening begun at 4.88nm before reducing gradually to 4.05nm with the increase in pump power. The former corresponds to a maximum of 6.3 times broadening ratio with respect to the pump linewidth. To date, this is the best achievement in the world at just below 1.7 W pump power level especially without utilizing pump-pulse synchronization or any external mode-locking modulations. In contrast without the tighter confinement geometry, the initiation of 4.25nm bandwidth was realized in the unstable power zone. These ascertain the double roles of dispersion compensating fiber as a stabilizing factor as well as for dispersion management.
format Article
author Sarmani, Abdul Rahman
Al-Alimi, Abdulmoghni Ali Wazae
Yusoff, N. Mohd
Mahdi, Mohd Adzir
spellingShingle Sarmani, Abdul Rahman
Al-Alimi, Abdulmoghni Ali Wazae
Yusoff, N. Mohd
Mahdi, Mohd Adzir
Spectral broadening in tight confinement geometry of a random fiber laser
author_facet Sarmani, Abdul Rahman
Al-Alimi, Abdulmoghni Ali Wazae
Yusoff, N. Mohd
Mahdi, Mohd Adzir
author_sort Sarmani, Abdul Rahman
title Spectral broadening in tight confinement geometry of a random fiber laser
title_short Spectral broadening in tight confinement geometry of a random fiber laser
title_full Spectral broadening in tight confinement geometry of a random fiber laser
title_fullStr Spectral broadening in tight confinement geometry of a random fiber laser
title_full_unstemmed Spectral broadening in tight confinement geometry of a random fiber laser
title_sort spectral broadening in tight confinement geometry of a random fiber laser
publisher Elsevier BV
publishDate 2022
url http://psasir.upm.edu.my/id/eprint/108727/1/Spectral%20broadening%20in%20tight%20confinement%20geometry%20of%20a%20random%20fiber%20laser.pdf
http://psasir.upm.edu.my/id/eprint/108727/
https://papers.ssrn.com/sol3/papers.cfm?abstract_id=4184332
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