2014
DOI: 10.7567/jjap.53.020301
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Octave spanning coherent supercontinuum generation using 51 fs high-power ultrashort pulse from Er-doped similariton amplifier

Abstract: A 51 fs, 4.4 nJ, almost-pedestal-free, high-power ultrashort pulse was generated using an Er-doped similariton amplifier. Using the generated ultrashort pulse, high-power, octave-spanning coherent supercontinua broadened from 1.05 to 2.15 and 0.95 to 2.3 µm were generated in highly nonlinear fibers. The characteristics of the similariton amplifier were investigated experimentally.

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Cited by 13 publications
(9 citation statements)
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“…By using ideal pedestal-free Raman shifted solitons in a highly nonlinear fiber (HNLF), they reported a high degree of flatness of 1 dB for a 520 nm SC bandwidth in the range from 1370 to 1890 nm [23]. Since then, many SC schemes with ultra-flat characteristics have been reported based on pedestal-free pump pulses in the normal and anomalous dispersion regimes [24][25][26][27][28]. Recently, mode-locked fiber laser (MLFLs) generating the so-called noise-like pulses (NLPs) have been proposed as the pump sources to realize spectral broadening in different kinds of optical fibers [29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…By using ideal pedestal-free Raman shifted solitons in a highly nonlinear fiber (HNLF), they reported a high degree of flatness of 1 dB for a 520 nm SC bandwidth in the range from 1370 to 1890 nm [23]. Since then, many SC schemes with ultra-flat characteristics have been reported based on pedestal-free pump pulses in the normal and anomalous dispersion regimes [24][25][26][27][28]. Recently, mode-locked fiber laser (MLFLs) generating the so-called noise-like pulses (NLPs) have been proposed as the pump sources to realize spectral broadening in different kinds of optical fibers [29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…24,25) We developed a highquality similariton amplifier based on the EDF system. 26) A parabolic-shaped, high power, almost ideal similariton pulse was generated in EDF. After the dispersion compensation, a 4.4 nJ, 51 fs, almost pedestal-free, high-power, ultrashort pulse was generated.…”
Section: Ultrashort Pulse Fiber Amplificationmentioning
confidence: 99%
“…Moreover, the single-mode fiber was used as an intermediate stage to convert laser pulse into Raman soliton centered at 1.67 μm, which was filtered with a low pass filter and used as the pump for SC generation process. The octave spanning supercontinuum was generated by Nozaki 18 in a dispersion shifted fiber (the spectrum from 0.95 μm to 2.30 μm and in a normal dispersion fiber (the spectrum from 1.05 μm to 2.15 μm). However, the presented system is not all-fiber again.…”
Section: Introductionmentioning
confidence: 99%