Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth
We investigated the effect of Rayleigh backscattering on the bandwidth of a multiwavelength random fiber laser (MWRFL). This MWRFL is based on an erbium-doped fiber amplifier (EDFA) as the gain medium and a Lyot filter as the wavelength-selective device. A high number and stable lasing line is gener...
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my.uniten.dspace-341342024-10-14T11:18:06Z Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth David A.P. Sulaiman A.H. Abdullah F. Ismail A. Jamaludin M.Z. Yusoff N.M. 57958805300 36810678100 56613644500 36023817800 58071849900 56036869700 erbium-doped fiber amplifier Lyot filter multiwavelength fiber laser nonlinear polarization rotation Backscattering Bandwidth Erbium doped fiber amplifiers Fiber lasers Light polarization Amplifier power Erbium-doped fiber amplifiers Half waveplate Lyot filters Multi wavelength fiber laser Multiwavelength Nonlinear polarization rotation Random fibers Rayleigh backscattering Single-mode fibers Single mode fibers We investigated the effect of Rayleigh backscattering on the bandwidth of a multiwavelength random fiber laser (MWRFL). This MWRFL is based on an erbium-doped fiber amplifier (EDFA) as the gain medium and a Lyot filter as the wavelength-selective device. A high number and stable lasing line is generated with the assistance of a nonlinear polarization rotation effect induced by highly nonlinear fiber (HNLF) and optimized by a polarization controller. Longer single-mode fiber (SMF) produces wider multiwavelength bandwidth as compared to shorter SMF lengths, as 10 km, 3 km, and 0.1 km obtained 6.24 nm, 5.76 nm, and 2.75 nm wavelength bandwidth, respectively. When the SMF is removed from the setup, no Rayleigh backscattering is provided in the cavity, which led to a narrower multiwavelength bandwidth of 2.69 nm. Subsequently, the alteration of EDFA power, half-wave plate (HWP) angle, and quarter-wave plate (QWP) angles affected the degradation of multiwavelength performance. The best output spectrum is achieved at an EDFA power of 18 dBm, a HWP angle of 60�, and a QWP angle of 105�. The laser stability over a period of 120 min was excellent with a peak power deviation of 1.33 dB. � 2023 IOP Publishing Ltd. Final 2024-10-14T03:18:06Z 2024-10-14T03:18:06Z 2023 Article 10.1088/1402-4896/acecbe 2-s2.0-85169578395 https://www.scopus.com/inward/record.uri?eid=2-s2.0-85169578395&doi=10.1088%2f1402-4896%2facecbe&partnerID=40&md5=f7cf128d0f48716acaad7859cc16c7fd https://irepository.uniten.edu.my/handle/123456789/34134 98 9 95023 Institute of Physics Scopus |
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erbium-doped fiber amplifier Lyot filter multiwavelength fiber laser nonlinear polarization rotation Backscattering Bandwidth Erbium doped fiber amplifiers Fiber lasers Light polarization Amplifier power Erbium-doped fiber amplifiers Half waveplate Lyot filters Multi wavelength fiber laser Multiwavelength Nonlinear polarization rotation Random fibers Rayleigh backscattering Single-mode fibers Single mode fibers |
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erbium-doped fiber amplifier Lyot filter multiwavelength fiber laser nonlinear polarization rotation Backscattering Bandwidth Erbium doped fiber amplifiers Fiber lasers Light polarization Amplifier power Erbium-doped fiber amplifiers Half waveplate Lyot filters Multi wavelength fiber laser Multiwavelength Nonlinear polarization rotation Random fibers Rayleigh backscattering Single-mode fibers Single mode fibers David A.P. Sulaiman A.H. Abdullah F. Ismail A. Jamaludin M.Z. Yusoff N.M. Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
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We investigated the effect of Rayleigh backscattering on the bandwidth of a multiwavelength random fiber laser (MWRFL). This MWRFL is based on an erbium-doped fiber amplifier (EDFA) as the gain medium and a Lyot filter as the wavelength-selective device. A high number and stable lasing line is generated with the assistance of a nonlinear polarization rotation effect induced by highly nonlinear fiber (HNLF) and optimized by a polarization controller. Longer single-mode fiber (SMF) produces wider multiwavelength bandwidth as compared to shorter SMF lengths, as 10 km, 3 km, and 0.1 km obtained 6.24 nm, 5.76 nm, and 2.75 nm wavelength bandwidth, respectively. When the SMF is removed from the setup, no Rayleigh backscattering is provided in the cavity, which led to a narrower multiwavelength bandwidth of 2.69 nm. Subsequently, the alteration of EDFA power, half-wave plate (HWP) angle, and quarter-wave plate (QWP) angles affected the degradation of multiwavelength performance. The best output spectrum is achieved at an EDFA power of 18 dBm, a HWP angle of 60�, and a QWP angle of 105�. The laser stability over a period of 120 min was excellent with a peak power deviation of 1.33 dB. � 2023 IOP Publishing Ltd. |
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57958805300 |
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57958805300 David A.P. Sulaiman A.H. Abdullah F. Ismail A. Jamaludin M.Z. Yusoff N.M. |
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David A.P. Sulaiman A.H. Abdullah F. Ismail A. Jamaludin M.Z. Yusoff N.M. |
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David A.P. |
title |
Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
title_short |
Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
title_full |
Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
title_fullStr |
Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
title_full_unstemmed |
Effect of Rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
title_sort |
effect of rayleigh backscattering on the multiwavelength random fiber laser bandwidth |
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Institute of Physics |
publishDate |
2024 |
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1814061042749145088 |
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13.214268 |