2017
DOI: 10.1109/jphot.2017.2679753
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Experimental Study of Output Characteristics of Bi-Directional Pumping High Power Fiber Amplifier in Different Pumping Schemes

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Cited by 41 publications
(36 citation statements)
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“…2(c), in which the forward pump power is 1336 W and the backward pump power is 2004 W (the ratio of the backward pump power to the total pump power is ∼60%). It is also noted that the slope efficiency under the counter-pump regime is higher than that under the co-pump and the bi-directional pump regime, which agrees with the reported results [34], [38]. However, with the forward pump power maintained and the backward pump power further increased, the output power continues to increase linearly while the threshold features in temporal and frequency domain are not strengthened.…”
Section: Experimental Investigationssupporting
confidence: 89%
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“…2(c), in which the forward pump power is 1336 W and the backward pump power is 2004 W (the ratio of the backward pump power to the total pump power is ∼60%). It is also noted that the slope efficiency under the counter-pump regime is higher than that under the co-pump and the bi-directional pump regime, which agrees with the reported results [34], [38]. However, with the forward pump power maintained and the backward pump power further increased, the output power continues to increase linearly while the threshold features in temporal and frequency domain are not strengthened.…”
Section: Experimental Investigationssupporting
confidence: 89%
“…For the monolithic fiber laser system, the investigation in experiment scope was less conducted. Shi et al have experimentally demonstrated the enhancement of the TMI threshold by changing pump direction [38], but the TMI threshold under counter-pump regime was proved lower than that under the co-pump regime, which run counter to the existing models and the underlying reason still needed to be explained. Meanwhile, the optimization of the forward and the backward pump allocation in bi-directional pump regime was not investigated in this work, and no theoretical model was provided to support all the experimental results, either.…”
Section: Introductionmentioning
confidence: 88%
“…Therefore, the seed power should not be too small and its optimization is indispensable in the designation of high-power fiber amplifiers. Moreover, it should be noted that the physical mechanism of weak-seed enhancement of SRS is not dependent on the type of active fiber, and the same phenomenon was witnessed in the double-cladding fiber laser with end-pumping technique [30].…”
Section: Resultsmentioning
confidence: 55%
“…However, Ref. [30] also observed that the Raman light will decrease with the increment of seed power, but no explanation was given. Besides, no other reference was found to report the phenomenon similar to Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Since the first publication of TMI in fiber laser systems 4 , lots of theoretical and experimental studies have been reported on TMI mitigation strategies 5 10 . Some conventional ways to avoid the TMI in high-power laser systems are to use extremely low NA fibers 11 , tight coiling 12 , 13 and controlling the heat load of the gain fiber by making a shift between the pumping wavelength and the gain fiber’s peak absorption wavelength 14 . Concerning the SRS, enlargement of the fiber mode area 15 , decreasing the effective fiber length, and broadening the bandwidth of fiber Bragg gratings (FBGs) 16 are the most common suppressing methods.…”
Section: Introductionmentioning
confidence: 99%