2018
DOI: 10.1088/1612-202x/aadfcd
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High-energy dissipative soliton-driven fiber optical parametric oscillator emitting at 1.7 µm

Abstract: We report a fiber optical parametric oscillator (FOPO) synchronously pumped in a C-band, delivering high-energy picosecond pulses exceeding the nanojoule level of around 1700 nm. The gain medium is a dispersion-shifted fiber, pumped by highly-chirped pulses from a mode-locked dissipative soliton fiber laser. Optimizing the pump wavelength along with time-dispersion-tuning of the FOPO enabled a broad tunability from 1617–1876 nm for the idler wave. In addition, relative intensity noise levels below  −140 dBc Hz… Show more

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Cited by 15 publications
(7 citation statements)
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“…Dissipative solitons are closely related to the high-energy pulses in the fiber lasers owing to its intrinsic feature. [256][257][258][259][260][261][262][263][264][265][266][267] As the development of the dissipative soliton research, an interesting pattern called dissipative soliton resonance (DSR) was reported. A DSR pulse is a complex of two interacting dissipative fronts.…”
Section: B Flat-top Dissipative Solitonmentioning
confidence: 99%
“…Dissipative solitons are closely related to the high-energy pulses in the fiber lasers owing to its intrinsic feature. [256][257][258][259][260][261][262][263][264][265][266][267] As the development of the dissipative soliton research, an interesting pattern called dissipative soliton resonance (DSR) was reported. A DSR pulse is a complex of two interacting dissipative fronts.…”
Section: B Flat-top Dissipative Solitonmentioning
confidence: 99%
“…However, the conversion efficiency of TDFs is relatively low due to strong reabsorption in the 1.7 μm band, while the preparation technology of BDFs and THDFs are not mature. The other is through nonlinear optical effects in solid-core fibers, including SRS [ 11 , 12 ], self-phase modulation [ 13 , 14 ], soliton self-frequency shift [ 15 , 16 ], and four-wave mixing [ 17 , 18 ], but the output laser linewidth is often wide. For some applications such as gas detection, narrow linewidth laser beams are needed to accurately distinguish the gas absorption lines, and a longer coherence length is also conducive to long-distance detection.…”
Section: Introductionmentioning
confidence: 99%
“…One is based on population inversion to generate 1.7 µm pulsed lasers by using rare-earth-doped fibers, such as thulium-doped fibers [6,7,10,11], thuliumholmium-codoped fibers [12,13], and bismuth-doped fibers [14][15][16]. The other is based on nonlinear effects in solid-core fibers to realize a frequency conversion, such as soliton self-frequency shift [17][18][19][20], four-wave mixing [21][22][23], self-phase modulation [7,24,25], and stimulated Raman scattering (SRS) [26]. Recently, fiber gas Raman lasers (FGRLs) based on hollow-core photonic crystal fibers (HC-PCFs) have opened a new opportunity for 1.7 µm pulsed fiber lasers [27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%