2016
DOI: 10.1364/oe.24.019940
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933 W Yb-doped fiber ASE amplifier with 504 nm bandwidth

Abstract: In this paper, a 933 W amplified spontaneous emission (ASE) source with a full width at half maximum (FWHM) of 50.4 nm is presented. The broadband source is generated by a 1271 W ASE amplifier together with 140m ordinary passive fiber for nonlinear transformation. With multi-wavelength rate equations and a nonlinear Schrödinger equation (NLSE), spectral evolution of the ASE source is analyzed theoretically.

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Cited by 23 publications
(5 citation statements)
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“…This is because when the pump light power is relatively low, the short wavelength ASE light will be reabsorbed as the pump light of the long wavelength ASE light, and the spectrum shows that the ASE light is concentrated in the long wavelength. With the increase in pump power, sufficient pump light can inhibit the reabsorption and make the ASE light at short wavelength increase rapidly, resulting in the overall ASE widening and the center wavelength shifting blue [22]. When the pump power is 7 W, the ASE spectrum is obtained by changing the length of the YDF to 3 m, 5 m, 7 m and 9 m, as shown in figure 3(b).…”
Section: Simulationmentioning
confidence: 99%
“…This is because when the pump light power is relatively low, the short wavelength ASE light will be reabsorbed as the pump light of the long wavelength ASE light, and the spectrum shows that the ASE light is concentrated in the long wavelength. With the increase in pump power, sufficient pump light can inhibit the reabsorption and make the ASE light at short wavelength increase rapidly, resulting in the overall ASE widening and the center wavelength shifting blue [22]. When the pump power is 7 W, the ASE spectrum is obtained by changing the length of the YDF to 3 m, 5 m, 7 m and 9 m, as shown in figure 3(b).…”
Section: Simulationmentioning
confidence: 99%
“…Thus, the nanosecond fiber seed generated by externally modulated SFS can resolve the temporal instability issues associated with the resonant cavity structure-based nanosecond fiber seed. However, demonstrations of high-power SFS amplifiers have predominantly focused on continuous-wave SFSs [22][23][24][25][26] , with reports on pulsed SFS amplifiers featuring high average power and large pulse energy being relatively scarce. Park et al [19] reported a narrowband nanosecond superfluorescent fiber source (ns-SFS) with an average power of 41.5 W, pulse energy of about 0.4 mJ and pulse width of 26.4 ns, while pulsed SFS amplifiers delivering average power at the hundred-watt level and pulse energy at the approximately 10 mJ level have yet to be reported.…”
Section: Introductionmentioning
confidence: 99%
“…In 2015, Xu et al obtained a kW-level SFS with 3 dB linewidth of ~8.1 nm through two stages of fiber amplifiers [12]. In 2016, Yan et al reported a 933 W SFS with 3 dB linewidth of as wide as ~50.4 nm by further performing nonlinear propagation in passive fiber [13]. In 2018, Xu et.al achieved a 3.14 kW SFS through tandem pump, and this is the highest reported output power in the fields of SFSs [14].…”
Section: Introductionmentioning
confidence: 99%