2016
DOI: 10.1364/oe.24.012072
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100 W dissipative soliton resonances from a thulium-doped double-clad all-fiber-format MOPA system

Abstract: In this paper, we first achieve nanosecond-scale dissipative soliton resonance (DSR) generation in a thulium-doped double-clad fiber (TDF) laser with all-anomalous-dispersion regime, and also first scale the average power up to 100.4 W by employing only two stage TDF amplifiers, corresponding to gains of 19.3 and 14.4 dB, respectively. It is noted that both the fiber laser oscillator and the amplification system employ double-clad fiber as the gain medium for utilizing the advantages in high-gain-availability,… Show more

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Cited by 95 publications
(43 citation statements)
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“…Thus, for too high an order of HML, the long trailing portion of the h-shaped pulses would fully occupy the pulse intervals, i.e., adjacent pulses would nearly overlap with each other. In the experimental aspect, however, the pulses would typically merge into a continuous wave operation rather than forming a pulse overlap state, like what we observed in our previous publication where the PDC could approach to 98.2% but its further increase would result in the transformation into a continuous wave state [34].…”
Section: B Ps-induced Switching Characteristicssupporting
confidence: 64%
See 1 more Smart Citation
“…Thus, for too high an order of HML, the long trailing portion of the h-shaped pulses would fully occupy the pulse intervals, i.e., adjacent pulses would nearly overlap with each other. In the experimental aspect, however, the pulses would typically merge into a continuous wave operation rather than forming a pulse overlap state, like what we observed in our previous publication where the PDC could approach to 98.2% but its further increase would result in the transformation into a continuous wave state [34].…”
Section: B Ps-induced Switching Characteristicssupporting
confidence: 64%
“…Relying on wavebreaking-free properties attributed to peak-power-clamping (PPC) effect, DSR has recently been shown as a promising mode-locking regime that could scale the pulse energy to virtually unlimited levels, and, in fact, up to 10 μJ single pulse energy from a fiber laser oscillator was achieved by G. Semaan et al [33]. The detailed amplifying characteristics of DSR pulses at 2 μm band were investigated by J. Zhao et al, where over 94 μJ amplified pulse energy was obtained with up to ~18.4 kW peak power from a thulium-doped fiber (TDF) master oscillator power amplifier (MOPA) system [34]. However, despite the unparalleled scalability in single pulse energy, the HML was still observed in the DSR regime [28,29,35].…”
Section: Introductionmentioning
confidence: 99%
“…As can be seen from Fig. 7, a signal amplification leads to a broadening of its spectrum 17 . To calculate pulse energy correctly, we have determined percentage of spectral power in the signal band.…”
Section: Resultsmentioning
confidence: 86%
“…Due to the low peak power, DSR pulses are perfect candidate for amplification. Amplified DSR pulses of tens of micro-Joules have been demonstrated [61]. DSR pulses can also be achieved in an all-polarization-maintaining fiber laser [62].…”
Section: Dissipative Soliton Generation In Fiber Lasersmentioning
confidence: 99%