2019
DOI: 10.1016/j.optlastec.2019.04.011
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Supercontinuum source based on all-silica fibers with optimized spectral power from 1100 up to 2300 nm

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Cited by 11 publications
(5 citation statements)
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“…The nominal dispersion of this ber at 1550 nm is null with a dispersion slope lower than 0.025 ps/(nm 2 • km) (with β 2 = 2.48•10 − 5 ps 2 /km and β 3 = − 2•10 − 6 ps 3 / km). The nonlinear coe cient is over 10 W − 1 /km and the Raman gain coe cient is higher than 4.8 W − 1 /km [20].…”
Section: Methodsmentioning
confidence: 90%
“…The nominal dispersion of this ber at 1550 nm is null with a dispersion slope lower than 0.025 ps/(nm 2 • km) (with β 2 = 2.48•10 − 5 ps 2 /km and β 3 = − 2•10 − 6 ps 3 / km). The nonlinear coe cient is over 10 W − 1 /km and the Raman gain coe cient is higher than 4.8 W − 1 /km [20].…”
Section: Methodsmentioning
confidence: 90%
“…The experimental set-up is based on a supercontinuum source introduced in ref. [5]. The supercontinuum is generated in a HNLF (Yangtze Optical Fibre and Cable Company Ltd., NL-1550-Zero type [6]) of 24 m length.…”
Section: Methodsmentioning
confidence: 99%
“…The output power is raised by means of a second amplifier (EDFA L26) with 26 dBm output saturation power (Manlight, model HWT-EDFA-GM-SC-BO-L26). The TDF sample amplifies a pulsed SC source, which is formed by an ultrafast erbium-doped fiber laser (EDFL) and a silica HNLF sample (YOFC, model NL1016-B) [17]. The EDFL is pulsed by passive mode-locking based on the NPR.…”
Section: Methodsmentioning
confidence: 99%