2016
DOI: 10.1364/oe.24.008708
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Investigation of stimulated Raman scattering effect in high-power fiber amplifiers seeded by narrow-band filtered superfluorescent source

Abstract: In this paper the stimulated Raman scattering (SRS) effect in high-power fiber amplifiers seeded by the narrow-band filtered superfluorescent source (SFS) is firstly analyzed both theoretically and experimentally. Spectral models for the formation of the SFS and the spectral evolution in high-power fiber amplifiers seeded by filtered SFS are proposed. It is found that the SRS effect in high-power fiber amplifiers depends on the spectral width of the filtered SFS seed. The theoretical predictions are in qualita… Show more

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Cited by 47 publications
(27 citation statements)
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“…Nowadays, filtered super-fluorescent source [2], multi-longitudinal-mode fiber oscillator [7][8][9], random fiber laser [10], fiber-Bragggrating-stabilized laser diode [11] and the phase modulated single frequency laser [4,5,[12][13][14][15] have been used as the narrow-linewidth injected seed in high power MOPA configurations. Among these different types, phase modulated single frequency laser has been proved to be preferable for the reason of stable temporal property, high SRS threshold and spectral purity during the amplification process [31][32][33]. Besides, stable temporal property and low intensity noise are also compatible with the TMI suppressing requirement of injected seed laser [19].…”
Section: Experimental Design Strateriesmentioning
confidence: 99%
“…Nowadays, filtered super-fluorescent source [2], multi-longitudinal-mode fiber oscillator [7][8][9], random fiber laser [10], fiber-Bragggrating-stabilized laser diode [11] and the phase modulated single frequency laser [4,5,[12][13][14][15] have been used as the narrow-linewidth injected seed in high power MOPA configurations. Among these different types, phase modulated single frequency laser has been proved to be preferable for the reason of stable temporal property, high SRS threshold and spectral purity during the amplification process [31][32][33]. Besides, stable temporal property and low intensity noise are also compatible with the TMI suppressing requirement of injected seed laser [19].…”
Section: Experimental Design Strateriesmentioning
confidence: 99%
“…[29] pumped by the LD. As the linewidth broadening is mainly induced by the generation of nonlinear effects [41] , such as self-phase modulation (SPM) and cross-phase modulation (XPM), the difference may be induced by the relative long gain fiber employed in this scheme. The spectral evolution in the power scaling process will be investigated in detail in the following paragraph.…”
Section: Resultsmentioning
confidence: 99%
“…The linear fitting result shown in Figure 4(c) indicates that the FWHM linewidth broadening factor of narrowband seed amplification increases with a rate of about 0.5952 nm per kilowatt, which is about 10 times as large as that of broadband seed amplification. This may be induced by the differences of the spectrum density and intensity noise of the seeds [41, 45, 46] . As the linewidth broadening in the narrowband seed amplification is relatively more serious than that in the broadband seed amplification, the optimization of the FWHM linewidth of the employed seed is very important for the design of the powerful SFS system if special output linewidth is required.…”
Section: Resultsmentioning
confidence: 99%
“…For core-pumped RFA, the typical pump sources are rare-earth doped fiber lasers, which induces strong temporal fluctuations in picosecond scale [19]. The spectral and temporal characteristics of this source can be calculated through combined simulation of the rate equations and nonlinear Shrödinger equations [20][21][22]. Here, we apply a simpler way to character the temporal fluctuations through the polarized thermal radiation model [23]:…”
Section: Spectral Broadening In a Single-frequency Rfamentioning
confidence: 99%