S-band multiwavelength Brillouin Raman Fiber Laser
In this paper we propose and demonstrate an S-band Brillouin-Raman Fiber Laser (BRFL). The S-band BRFL utilizes a Dispersion Compensating Fiber (DCF) as the non-linear gain medium in a linear cavity configuration and amplified by two 1425 nm, 380 mW pumped Raman Fiber Amplifiers (RFAs). A Brillouin...
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my.um.eprints.198682019-01-02T03:25:36Z http://eprints.um.edu.my/19868/ S-band multiwavelength Brillouin Raman Fiber Laser Ahmad, Harith Zulkifli, Mohd Zamani Norizan, Siti Fatimah Jemangin, M.H. Harun, Sulaiman Wadi QC Physics TK Electrical engineering. Electronics Nuclear engineering In this paper we propose and demonstrate an S-band Brillouin-Raman Fiber Laser (BRFL). The S-band BRFL utilizes a Dispersion Compensating Fiber (DCF) as the non-linear gain medium in a linear cavity configuration and amplified by two 1425 nm, 380 mW pumped Raman Fiber Amplifiers (RFAs). A Brillouin Pump (BP) signal of 1515 nm at 12 dBm in power is injected into the setup to generate Stokes lines via the Stimulated Brillouin Scattering (SBS) process. The S-band BRFL is able of generating a Brillouin comb with 32 Stokes lines with a flat peak output power of - 18 dBm. The best BP to Stokes power ratio of the system is determined to be 50:50, while a ratio of 70:30 is observed to generate Stokes with a higher peak power, but at the expense of the number of wavelengths. The S-band BRFL has many potential applications as multiwavelength sources for communications and sensors. Elsevier 2011 Article PeerReviewed Ahmad, Harith and Zulkifli, Mohd Zamani and Norizan, Siti Fatimah and Jemangin, M.H. and Harun, Sulaiman Wadi (2011) S-band multiwavelength Brillouin Raman Fiber Laser. Optics Communications, 284 (20). pp. 4971-4974. ISSN 0030-4018 https://doi.org/10.1016/j.optcom.2011.06.048 doi:10.1016/j.optcom.2011.06.048 |
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QC Physics TK Electrical engineering. Electronics Nuclear engineering Ahmad, Harith Zulkifli, Mohd Zamani Norizan, Siti Fatimah Jemangin, M.H. Harun, Sulaiman Wadi S-band multiwavelength Brillouin Raman Fiber Laser |
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In this paper we propose and demonstrate an S-band Brillouin-Raman Fiber Laser (BRFL). The S-band BRFL utilizes a Dispersion Compensating Fiber (DCF) as the non-linear gain medium in a linear cavity configuration and amplified by two 1425 nm, 380 mW pumped Raman Fiber Amplifiers (RFAs). A Brillouin Pump (BP) signal of 1515 nm at 12 dBm in power is injected into the setup to generate Stokes lines via the Stimulated Brillouin Scattering (SBS) process. The S-band BRFL is able of generating a Brillouin comb with 32 Stokes lines with a flat peak output power of - 18 dBm. The best BP to Stokes power ratio of the system is determined to be 50:50, while a ratio of 70:30 is observed to generate Stokes with a higher peak power, but at the expense of the number of wavelengths. The S-band BRFL has many potential applications as multiwavelength sources for communications and sensors. |
format |
Article |
author |
Ahmad, Harith Zulkifli, Mohd Zamani Norizan, Siti Fatimah Jemangin, M.H. Harun, Sulaiman Wadi |
author_facet |
Ahmad, Harith Zulkifli, Mohd Zamani Norizan, Siti Fatimah Jemangin, M.H. Harun, Sulaiman Wadi |
author_sort |
Ahmad, Harith |
title |
S-band multiwavelength Brillouin Raman Fiber Laser |
title_short |
S-band multiwavelength Brillouin Raman Fiber Laser |
title_full |
S-band multiwavelength Brillouin Raman Fiber Laser |
title_fullStr |
S-band multiwavelength Brillouin Raman Fiber Laser |
title_full_unstemmed |
S-band multiwavelength Brillouin Raman Fiber Laser |
title_sort |
s-band multiwavelength brillouin raman fiber laser |
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Elsevier |
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2011 |
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http://eprints.um.edu.my/19868/ https://doi.org/10.1016/j.optcom.2011.06.048 |
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1643691111904968704 |