International Photonics and OptoElectronics Meetings 2014
DOI: 10.1364/fbta.2014.ff4b.1
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A 1.3 kW Raman fiber laser

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Cited by 3 publications
(3 citation statements)
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“…The numerical aperture is 0.275, which corresponds to a peak refractive-index difference to the pure-silica cladding of 0.026. From this, the Raman gain coefficient g R can be estimated to 1.19 × 10 −13 m/W in the center of the core for unpolarised light at 975 nm [10,11]. The propagation loss was measured to 1.7 dB/km at the pump wavelength and 1.5 dB/km at the Stokes wavelength of 1019 nm.…”
Section: Multimode Raman Gain Fibermentioning
confidence: 99%
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“…The numerical aperture is 0.275, which corresponds to a peak refractive-index difference to the pure-silica cladding of 0.026. From this, the Raman gain coefficient g R can be estimated to 1.19 × 10 −13 m/W in the center of the core for unpolarised light at 975 nm [10,11]. The propagation loss was measured to 1.7 dB/km at the pump wavelength and 1.5 dB/km at the Stokes wavelength of 1019 nm.…”
Section: Multimode Raman Gain Fibermentioning
confidence: 99%
“…As an example, a YDFL-pumped fiber Raman laser reached 1.3 kW of CW output power at 1120 nm with high overall conversion efficiency [11]. Still, the use of a two-stage pumping scheme makes the FRLs more complex and is only practical for certain wavelengths.…”
Section: Introductionmentioning
confidence: 99%
“…Raman fiber lasers have gained attention in recent years due to their broad gain bandwidth and wavelength-insensitive pumping [1][2][3][4][5][6][7]. With low heat loads due to the inherently small quantum defect and long fiber lengths, they are expected to be highly resistant to thermal degradation and transverse modal instabilities (TMI) [1,4,8].…”
Section: Introductionmentioning
confidence: 99%